| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
actuator (alpha) | Generic simple description of a heating/current drive actuator, for a first simplified version of the Plasma Simulator component | |||
actuator.channels (alpha) | [1...N] | STR_1D | ID of the multiple channels of the actuator: Beam boxes for NBI, EC or IC launcher, ... | |
actuator.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
actuator.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
actuator.code.name (alpha) | STR_0D | Name of software generating IDS | ||
actuator.code.output_flag (alpha) | [actuator.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
actuator.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
actuator.code.repository (alpha) | STR_0D | URL of software repository | ||
actuator.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
actuator.generic_dynamic (alpha) | [actuator.channels, | FLT_2D (uncertain) | mixed | Generic 2D dynamic slot for storing an actuator control parameter (e.g. the angle of an ECRH mirror) |
actuator.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
actuator.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
actuator.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
actuator.name (alpha) | STR_0D | - | Name of the actuator (IC, EC, NBI, LH) | |
actuator.power (alpha) | [actuator.channels, | FLT_2D (uncertain) | W | Power delivered at the output of the actuator, in the vessel (NB this is before the coupling / beam blocking / shine through / orbit losses calculations) |
actuator.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
amns_data (alpha) | Atomic, molecular, nuclear and surface physics data. Each occurrence contains the data for a given element (nuclear charge), describing various physical processes. For each process, data tables are organized by charge states. The coordinate system used by the data tables is described under the coordinate_system node. | |||
amns_data.a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
amns_data.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
amns_data.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
amns_data.code.name (alpha) | STR_0D | Name of software generating IDS | ||
amns_data.code.output_flag (alpha) | [amns_data.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
amns_data.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
amns_data.code.repository (alpha) | STR_0D | URL of software repository | ||
amns_data.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
amns_data.coordinate_system (alpha) | [1...N] | STRUCT_ARRAY | Array of possible coordinate systems for process tables | |
amns_data.coordinate_system[:].coordinate (alpha) | [1...N] | STRUCT_ARRAY | Set of coordinates for that coordinate system. A coordinate an be either a range of real values or a set of discrete values (if interpolation_type=0) | |
amns_data.coordinate_system[:].coordinate[:].extrapolation_type (alpha) | [1...2] | INT_1D | Extrapolation strategy when leaving the domain. The first value of the vector describes the behaviour at lower bound, the second describes the at upper bound. Possible values: 0=none, report error; 1=boundary value; 2=linear extrapolation | |
amns_data.coordinate_system[:].coordinate[:].interpolation_type (alpha) | INT_0D | Interpolation strategy in this coordinate direction. Integer flag: 0=discrete (no interpolation); 1=linear; ... | ||
amns_data.coordinate_system[:].coordinate[:].label (alpha) | STR_0D | Description of coordinate (e.g. "Electron temperature") | ||
amns_data.coordinate_system[:].coordinate[:].spacing (alpha) | INT_0D | Flag for specific coordinate spacing (for optimization purposes). Integer flag: 0=undefined; 1=uniform; ... | ||
amns_data.coordinate_system[:].coordinate[:].transformation (alpha) | INT_0D | Coordinate transformation applied to coordinate values stored in coord. Integer flag: 0=none; 1=log10; 2=ln | ||
amns_data.coordinate_system[:].coordinate[:].units (alpha) | STR_0D | Units of coordinate (e.g. eV) | ||
amns_data.coordinate_system[:].coordinate[:].value_labels (alpha) | [amns_data.coordinate_system[:].coordinate[:].values] | STR_1D | String description of discrete coordinate values (if interpolation_type=0). E.g., for spectroscopic lines, the spectroscopic description of the transition. | |
amns_data.coordinate_system[:].coordinate[:].values (alpha) | [1...N] | FLT_1D (uncertain) | units given by coordinate_system(:)/coordinate(:)/units | Coordinate values |
amns_data.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
amns_data.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
amns_data.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
amns_data.ids_properties.occurrence | INT_0D | |||
amns_data.process (alpha) | [1...N] | STRUCT_ARRAY | Description and data for a set of physical processes. | |
amns_data.process[:].charge_state (alpha) | [1...N] | STRUCT_ARRAY | Process tables for a set of charge states. Only one table is used for that process, defined by process(:)/table_dimension | |
amns_data.process[:].charge_state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
amns_data.process[:].charge_state[:].table_0d (alpha) | FLT_0D (uncertain) | units given by process(:)/results_units | 0D table describing the process data | |
amns_data.process[:].charge_state[:].table_1d (alpha) | [amns_data.process[:].charge_state[:].table_1d.coordinate_system[:].coordinate] | FLT_1D (uncertain) | units given by process(:)/results_units | 1D table describing the process data |
amns_data.process[:].charge_state[:].table_2d (alpha) | [amns_data.process[:].charge_state[:].table_2d.coordinate_system[:].coordinate, | FLT_2D (uncertain) | units given by process(:)/results_units | 2D table describing the process data |
amns_data.process[:].charge_state[:].table_3d (alpha) | [amns_data.process[:].charge_state[:].table_3d.coordinate_system[:].coordinate, | FLT_3D (uncertain) | units given by process(:)/results_units | 3D table describing the process data |
amns_data.process[:].charge_state[:].table_4d (alpha) | [amns_data.process[:].charge_state[:].table_4d.coordinate_system[:].coordinate, | FLT_4D (uncertain) | units given by process(:)/results_units | 4D table describing the process data |
amns_data.process[:].charge_state[:].table_5d (alpha) | [amns_data.process[:].charge_state[:].table_5d.coordinate_system[:].coordinate, | FLT_5D (uncertain) | units given by process(:)/results_units | 5D table describing the process data |
amns_data.process[:].charge_state[:].table_6d (alpha) | [amns_data.process[:].charge_state[:].table_6d.coordinate_system[:].coordinate, | FLT_6D (uncertain) | units given by process(:)/results_units | 6D table describing the process data |
amns_data.process[:].charge_state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
amns_data.process[:].charge_state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
amns_data.process[:].coordinate_index (alpha) | INT_0D | Index in tables_coord, specifying what coordinate systems to use for this process (valid for all tables) | ||
amns_data.process[:].label (alpha) | STR_0D | String identifying the process (e.g. EI, RC, ...) | ||
amns_data.process[:].products (alpha) | [1...N] | STRUCT_ARRAY | Set of products resulting of this process | |
amns_data.process[:].products[:].charge (alpha) | FLT_0D (uncertain) | - | Charge number of the participant | |
amns_data.process[:].products[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom (in such cas, this array should be of size 1) or molecule | |
amns_data.process[:].products[:].element[:].a (alpha) | INT_0D | Atomic Mass Unit | Number of nucleons in the nucleus (nuclear mass); 0 if none (e-, gamma); Not set if not important (e.g. for an atomic process that is not isotope dependent) | |
amns_data.process[:].products[:].element[:].label (alpha) | STR_0D | String identifier for reaction constituent (e.g. "D", "C") | ||
amns_data.process[:].products[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom in the molecule | |
amns_data.process[:].products[:].element[:].z_n (alpha) | INT_0D | Elementary Charge Unit | Nuclear charge. 0 if none (e-, gamma) | |
amns_data.process[:].products[:].label (alpha) | STR_0D | String identifying reaction participant (e.g. "D", "e", "W", "CD4", "photon", "n") | ||
amns_data.process[:].products[:].mass (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of the participant | |
amns_data.process[:].products[:].metastable (alpha) | [1...N] | INT_1D | An array identifying the metastable; if zero-length, then not a metastable; if of length 1, then the value indicates the electronic level for the metastable (mostly used for atoms/ions); if of length 2, then the 1st would indicate the electronic level and the second the vibrational level for the metastable (mostly used for molecules and molecular ions); if of length 3, then the 1st would indicate the electronic level, the second the vibrational level and the third the rotational level for the metastable (mostly used for molecules and molecular ions) | |
amns_data.process[:].products[:].metastable_label (alpha) | STR_0D | Label identifying in text form the metastable | ||
amns_data.process[:].products[:].multiplicity (alpha) | FLT_0D (uncertain) | - | Multiplicity in the reaction | |
amns_data.process[:].products[:].relative_charge (alpha) | INT_0D | This is a flag indicating that charges are absolute (if set to 0), relative (if 1) or irrelevant (-1); relative would be used to categorize the ionization reactions from i to i+1 for all charge states; in the case of bundles, the +1 relative indicates the next bundle | ||
amns_data.process[:].products[:].role (alpha) | STRUCTURE | Identifier for the role of this paricipant in the reaction. For surface reactions distinguish between projectile and wall. | ||
amns_data.process[:].products[:].role.description (alpha) | STR_0D | Verbose description | ||
amns_data.process[:].products[:].role.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
amns_data.process[:].products[:].role.name (alpha) | STR_0D | Short string identifier | ||
amns_data.process[:].reactants (alpha) | [1...N] | STRUCT_ARRAY | Set of reactants involved in this process | |
amns_data.process[:].reactants[:].charge (alpha) | FLT_0D (uncertain) | - | Charge number of the participant | |
amns_data.process[:].reactants[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom (in such cas, this array should be of size 1) or molecule | |
amns_data.process[:].reactants[:].element[:].a (alpha) | INT_0D | Atomic Mass Unit | Number of nucleons in the nucleus (nuclear mass); 0 if none (e-, gamma); Not set if not important (e.g. for an atomic process that is not isotope dependent) | |
amns_data.process[:].reactants[:].element[:].label (alpha) | STR_0D | String identifier for reaction constituent (e.g. "D", "C") | ||
amns_data.process[:].reactants[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom in the molecule | |
amns_data.process[:].reactants[:].element[:].z_n (alpha) | INT_0D | Elementary Charge Unit | Nuclear charge. 0 if none (e-, gamma) | |
amns_data.process[:].reactants[:].label (alpha) | STR_0D | String identifying reaction participant (e.g. "D", "e", "W", "CD4", "photon", "n") | ||
amns_data.process[:].reactants[:].mass (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of the participant | |
amns_data.process[:].reactants[:].metastable (alpha) | [1...N] | INT_1D | An array identifying the metastable; if zero-length, then not a metastable; if of length 1, then the value indicates the electronic level for the metastable (mostly used for atoms/ions); if of length 2, then the 1st would indicate the electronic level and the second the vibrational level for the metastable (mostly used for molecules and molecular ions); if of length 3, then the 1st would indicate the electronic level, the second the vibrational level and the third the rotational level for the metastable (mostly used for molecules and molecular ions) | |
amns_data.process[:].reactants[:].metastable_label (alpha) | STR_0D | Label identifying in text form the metastable | ||
amns_data.process[:].reactants[:].multiplicity (alpha) | FLT_0D (uncertain) | - | Multiplicity in the reaction | |
amns_data.process[:].reactants[:].relative_charge (alpha) | INT_0D | This is a flag indicating that charges are absolute (if set to 0), relative (if 1) or irrelevant (-1); relative would be used to categorize the ionization reactions from i to i+1 for all charge states; in the case of bundles, the +1 relative indicates the next bundle | ||
amns_data.process[:].reactants[:].role (alpha) | STRUCTURE | Identifier for the role of this paricipant in the reaction. For surface reactions distinguish between projectile and wall. | ||
amns_data.process[:].reactants[:].role.description (alpha) | STR_0D | Verbose description | ||
amns_data.process[:].reactants[:].role.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
amns_data.process[:].reactants[:].role.name (alpha) | STR_0D | Short string identifier | ||
amns_data.process[:].result_label (alpha) | STR_0D | Description of the process result (rate, cross section, sputtering yield, ...) | ||
amns_data.process[:].result_transformation (alpha) | INT_0D | Transformation of the process result. Integer flag: 0=no transformation; 1=10^; 2=exp() | ||
amns_data.process[:].result_units (alpha) | STR_0D | Units of the process result | ||
amns_data.process[:].table_dimension (alpha) | INT_0D | Table dimensionality of the process (1 to 6), valid for all charge states. Indicates which of the tables is filled (below the charge_state node) | ||
amns_data.release (alpha) | [1...N] | STRUCT_ARRAY | List of available releases of the AMNS data; each element contains information about the AMNS data that is included in the release. This part of the IDS is filled and stored only into shot/run=0/1, playing the role of a catalogue. | |
amns_data.release[:].data_entry (alpha) | [1...N] | STRUCT_ARRAY | For this release, list of each data item (i.e. shot/run pair containing the actual data) included in this release | |
amns_data.release[:].data_entry[:].description (alpha) | STR_0D | Description of this data entry | ||
amns_data.release[:].data_entry[:].run (alpha) | INT_0D | Which run number is the active run number for this version | ||
amns_data.release[:].data_entry[:].shot (alpha) | INT_0D | Shot number = Mass*100+Nuclear_charge | ||
amns_data.release[:].date (alpha) | STR_0D | Date of this release | ||
amns_data.release[:].description (alpha) | STR_0D | Description of this release | ||
amns_data.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
amns_data.z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
bolometer (alpha) | Bolometer diagnostic | |||
bolometer.channel (alpha) | [1...N] | STRUCT_ARRAY | Set of channels (lines-of-sight) | |
bolometer.channel[:].aperture (alpha) | [1...N] | STRUCT_ARRAY | Description of a set of collimating apertures | |
bolometer.channel[:].aperture[:].origin (alpha) | STRUCTURE | Origin of the local coordinate system (X1,X2,X3) describing the plane detector/aperture. This origin is located within the detector/aperture area. The X1 axis is horizontal and oriented is the positive phi direction (counter-clockwise when seen from above). The X3 axis is normal to the detector/aperture plane and oriented towards the plasma. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
bolometer.channel[:].aperture[:].origin.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
bolometer.channel[:].aperture[:].origin.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
bolometer.channel[:].aperture[:].origin.z (alpha) | FLT_0D (uncertain) | m | Height | |
bolometer.channel[:].aperture[:].outline (alpha) | STRUCTURE | Irregular outline of the detector/aperture in the (X1, X2) coordinate system | ||
bolometer.channel[:].aperture[:].outline.x1 (alpha) | [1...N] | FLT_1D (uncertain) | m | Positions along x1 axis |
bolometer.channel[:].aperture[:].outline.x2 (alpha) | [bolometer.channel[:].aperture[:].outline.x1] | FLT_1D (uncertain) | m | Positions along x2 axis |
bolometer.channel[:].aperture[:].x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. | ||
bolometer.channel[:].aperture[:].x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
bolometer.channel[:].aperture[:].x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
bolometer.channel[:].aperture[:].x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
bolometer.channel[:].aperture[:].x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. | ||
bolometer.channel[:].aperture[:].x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
bolometer.channel[:].aperture[:].x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
bolometer.channel[:].aperture[:].x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
bolometer.channel[:].aperture[:].x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. | ||
bolometer.channel[:].aperture[:].x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
bolometer.channel[:].aperture[:].x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
bolometer.channel[:].aperture[:].x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
bolometer.channel[:].detector (alpha) | STRUCTURE | Detector description | ||
bolometer.channel[:].detector.origin (alpha) | STRUCTURE | Origin of the local coordinate system (X1,X2,X3) describing the plane detector/aperture. This origin is located within the detector/aperture area. The X1 axis is horizontal and oriented is the positive phi direction (counter-clockwise when seen from above). The X3 axis is normal to the detector/aperture plane and oriented towards the plasma. The X2 axis is orthonormal so that uX2 = uX3 x uX1. | ||
bolometer.channel[:].detector.origin.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
bolometer.channel[:].detector.origin.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
bolometer.channel[:].detector.origin.z (alpha) | FLT_0D (uncertain) | m | Height | |
bolometer.channel[:].detector.outline (alpha) | STRUCTURE | Irregular outline of the detector/aperture in the (X1, X2) coordinate system | ||
bolometer.channel[:].detector.outline.x1 (alpha) | [1...N] | FLT_1D (uncertain) | m | Positions along x1 axis |
bolometer.channel[:].detector.outline.x2 (alpha) | [bolometer.channel[:].detector.outline.x1] | FLT_1D (uncertain) | m | Positions along x2 axis |
bolometer.channel[:].detector.x1_unit_vector (alpha) | STRUCTURE | Components of the X1 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. | ||
bolometer.channel[:].detector.x1_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
bolometer.channel[:].detector.x1_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
bolometer.channel[:].detector.x1_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
bolometer.channel[:].detector.x2_unit_vector (alpha) | STRUCTURE | Components of the X2 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. | ||
bolometer.channel[:].detector.x2_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
bolometer.channel[:].detector.x2_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
bolometer.channel[:].detector.x2_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
bolometer.channel[:].detector.x3_unit_vector (alpha) | STRUCTURE | Components of the X3 direction unit vector in the (X,Y,Z) coordinate system, where X is the major radius axis for phi = 0, Y is the major radius axis for phi = pi/2, and Z is the height axis. | ||
bolometer.channel[:].detector.x3_unit_vector.x (alpha) | FLT_0D (uncertain) | m | Component along X axis | |
bolometer.channel[:].detector.x3_unit_vector.y (alpha) | FLT_0D (uncertain) | m | Component along Y axis | |
bolometer.channel[:].detector.x3_unit_vector.z (alpha) | FLT_0D (uncertain) | m | Component along Z axis | |
bolometer.channel[:].identifier (alpha) | STR_0D | ID of the channel | ||
bolometer.channel[:].line_of_sight (alpha) | STRUCTURE | Description of the reference line of sight of the channel, defined by two points when the beam is not reflected, a third point is added to define the reflected beam path | ||
bolometer.channel[:].line_of_sight.first_point (alpha) | STRUCTURE | Position of the first point | ||
bolometer.channel[:].line_of_sight.first_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
bolometer.channel[:].line_of_sight.first_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
bolometer.channel[:].line_of_sight.first_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
bolometer.channel[:].line_of_sight.second_point (alpha) | STRUCTURE | Position of the second point | ||
bolometer.channel[:].line_of_sight.second_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
bolometer.channel[:].line_of_sight.second_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
bolometer.channel[:].line_of_sight.second_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
bolometer.channel[:].line_of_sight.third_point (alpha) | STRUCTURE | Position of the third point | ||
bolometer.channel[:].line_of_sight.third_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
bolometer.channel[:].line_of_sight.third_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
bolometer.channel[:].line_of_sight.third_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
bolometer.channel[:].name (alpha) | STR_0D | Name of the channel | ||
bolometer.channel[:].power (alpha) | STRUCTURE | Power received on the detector | ||
bolometer.channel[:].power.data (alpha) | [bolometer.channel[:].power.time] | FLT_1D (uncertain) | W | Power received on the detector |
bolometer.channel[:].power.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
bolometer.channel[:].validity (alpha) | INT_0D | Indicator of the validity of the channel for the whole acquisition period (0 means valid, negative values mean non-valid) | ||
bolometer.channel[:].validity_timed (alpha) | STRUCTURE | Indicator of the validity of the channel as a function of time (0 means valid, negative values mean non-valid) | ||
bolometer.channel[:].validity_timed.data (alpha) | [bolometer.channel[:].validity_timed.time] | INT_1D | Indicator of the validity of the channel as a function of time (0 means valid, negative values mean non-valid) | |
bolometer.channel[:].validity_timed.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
bolometer.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
bolometer.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
bolometer.code.name (alpha) | STR_0D | Name of software generating IDS | ||
bolometer.code.output_flag (alpha) | [bolometer.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
bolometer.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
bolometer.code.repository (alpha) | STR_0D | URL of software repository | ||
bolometer.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
bolometer.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
bolometer.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
bolometer.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
bolometer.ids_properties.occurrence | INT_0D | |||
bolometer.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
charge_exchange (alpha) | Charge exchange spectroscopy diagnostic | |||
charge_exchange.channel (alpha) | [1...N] | STRUCT_ARRAY | Set of channels (lines-of-sight) | |
charge_exchange.channel[:].a (alpha) | [charge_exchange.channel[:].channel_names] | FLT_1D (uncertain) | Atomic Mass Unit | Mass of atom of the emmitting impurity. Varies according to channels since they are spanning different lines of sight |
charge_exchange.channel[:].identifier (alpha) | STR_0D | ID of the channel | ||
charge_exchange.channel[:].label (alpha) | [charge_exchange.channel[:].channel_names] | STR_1D | String identifying the emmitting impurity (e.g. H+, D+, T+, He+2, C+6, ...) | |
charge_exchange.channel[:].name (alpha) | STR_0D | Name of the channel | ||
charge_exchange.channel[:].position (alpha) | STRUCTURE | Position of the measurements | ||
charge_exchange.channel[:].position.phi (alpha) | STRUCTURE | Toroidal angle | ||
charge_exchange.channel[:].position.phi.data (alpha) | [charge_exchange.channel[:].position.phi.time] | FLT_1D (uncertain) | rad | Toroidal angle |
charge_exchange.channel[:].position.phi.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
charge_exchange.channel[:].position.r (alpha) | STRUCTURE | Major radius | ||
charge_exchange.channel[:].position.r.data (alpha) | [charge_exchange.channel[:].position.r.time] | FLT_1D (uncertain) | m | Major radius |
charge_exchange.channel[:].position.r.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
charge_exchange.channel[:].position.z (alpha) | STRUCTURE | Height | ||
charge_exchange.channel[:].position.z.data (alpha) | [charge_exchange.channel[:].position.z.time] | FLT_1D (uncertain) | m | Height |
charge_exchange.channel[:].position.z.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
charge_exchange.channel[:].temperature (alpha) | STRUCTURE | Ion temperature (of the emmitting impurity) | ||
charge_exchange.channel[:].temperature.data (alpha) | [charge_exchange.channel[:].temperature.time] | FLT_1D (uncertain) | eV | Ion temperature (of the emmitting impurity) |
charge_exchange.channel[:].temperature.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
charge_exchange.channel[:].velocity_pol (alpha) | STRUCTURE | Poloidal velocity (of the emmitting impurity) | ||
charge_exchange.channel[:].velocity_pol.data (alpha) | [charge_exchange.channel[:].velocity_pol.time] | FLT_1D (uncertain) | eV | Poloidal velocity (of the emmitting impurity) |
charge_exchange.channel[:].velocity_pol.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
charge_exchange.channel[:].velocity_tor (alpha) | STRUCTURE | Toroidal velocity (of the emmitting impurity) | ||
charge_exchange.channel[:].velocity_tor.data (alpha) | [charge_exchange.channel[:].velocity_tor.time] | FLT_1D (uncertain) | eV | Toroidal velocity (of the emmitting impurity) |
charge_exchange.channel[:].velocity_tor.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
charge_exchange.channel[:].z_ion (alpha) | [charge_exchange.channel[:].channel_names] | FLT_1D (uncertain) | Elementary Charge Unit | Ion charge of the emmitting impurity. Varies according to channels since they are spanning different lines of sight |
charge_exchange.channel[:].z_n (alpha) | [charge_exchange.channel[:].channel_names] | FLT_1D (uncertain) | Elementary Charge Unit | Nuclear charge of the emmitting impurity. Varies according to channels since they are spanning different lines of sight |
charge_exchange.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
charge_exchange.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
charge_exchange.code.name (alpha) | STR_0D | Name of software generating IDS | ||
charge_exchange.code.output_flag (alpha) | [charge_exchange.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
charge_exchange.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
charge_exchange.code.repository (alpha) | STR_0D | URL of software repository | ||
charge_exchange.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
charge_exchange.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
charge_exchange.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
charge_exchange.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
charge_exchange.ids_properties.occurrence | INT_0D | |||
charge_exchange.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
controllers (alpha) | Feedback and feedforward controllers | |||
controllers.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
controllers.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
controllers.code.name (alpha) | STR_0D | Name of software generating IDS | ||
controllers.code.output_flag (alpha) | [controllers.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
controllers.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
controllers.code.repository (alpha) | STR_0D | URL of software repository | ||
controllers.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
controllers.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
controllers.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
controllers.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
controllers.ids_properties.occurrence | INT_0D | |||
controllers.linear_controller (alpha) | [1...N] | STRUCT_ARRAY | A linear controller, this is rather conventional | |
controllers.linear_controller[:].controller_class (alpha) | STR_0D | One of a known class of controllers | ||
controllers.linear_controller[:].description (alpha) | STR_0D | Description of this controller | ||
controllers.linear_controller[:].input_names (alpha) | [1...N] | STR_1D | Names of the input signals, following the SDN convention | |
controllers.linear_controller[:].inputs (alpha) | STRUCTURE | Input signals; the timebase is common to inputs and outputs for any particular controller | ||
controllers.linear_controller[:].inputs.data (alpha) | [controllers.linear_controller[:].input_names, | FLT_2D (uncertain) | mixed | Input signals; the timebase is common to inputs and outputs for any particular controller |
controllers.linear_controller[:].inputs.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].name (alpha) | STR_0D | Name of this controller | ||
controllers.linear_controller[:].output_names (alpha) | [1...N] | STR_1D | Names of the output signals following the SDN convention | |
controllers.linear_controller[:].outputs (alpha) | STRUCTURE | Output signals; the timebase is common to inputs and outputs for any particular controller | ||
controllers.linear_controller[:].outputs.data (alpha) | [controllers.linear_controller[:].output_names, | FLT_2D (uncertain) | mixed | Output signals; the timebase is common to inputs and outputs for any particular controller |
controllers.linear_controller[:].outputs.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].pid (alpha) | STRUCTURE | Filtered PID controller | ||
controllers.linear_controller[:].pid.d (alpha) | STRUCTURE | Derivative term | ||
controllers.linear_controller[:].pid.d.data (alpha) | [controllers.linear_controller[:].pid.output_names, | FLT_3D (uncertain) | mixed | Derivative term |
controllers.linear_controller[:].pid.d.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].pid.i (alpha) | STRUCTURE | Integral term | ||
controllers.linear_controller[:].pid.i.data (alpha) | [controllers.linear_controller[:].pid.output_names, | FLT_3D (uncertain) | mixed | Integral term |
controllers.linear_controller[:].pid.i.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].pid.p (alpha) | STRUCTURE | Proportional term | ||
controllers.linear_controller[:].pid.p.data (alpha) | [controllers.linear_controller[:].pid.output_names, | FLT_3D (uncertain) | mixed | Proportional term |
controllers.linear_controller[:].pid.p.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].pid.tau (alpha) | STRUCTURE | Filter time-constant for the D-term | ||
controllers.linear_controller[:].pid.tau.data (alpha) | [controllers.linear_controller[:].pid.tau.time] | FLT_1D (uncertain) | s | Filter time-constant for the D-term |
controllers.linear_controller[:].pid.tau.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].statespace (alpha) | STRUCTURE | Statespace controller in discrete or continuous time | ||
controllers.linear_controller[:].statespace.a (alpha) | STRUCTURE | A matrix | ||
controllers.linear_controller[:].statespace.a.data (alpha) | [controllers.linear_controller[:].statespace.state_names, | FLT_3D (uncertain) | mixed | A matrix |
controllers.linear_controller[:].statespace.a.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].statespace.b (alpha) | STRUCTURE | B matrix | ||
controllers.linear_controller[:].statespace.b.data (alpha) | [controllers.linear_controller[:].statespace.state_names, | FLT_3D (uncertain) | mixed | B matrix |
controllers.linear_controller[:].statespace.b.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].statespace.c (alpha) | STRUCTURE | C matrix | ||
controllers.linear_controller[:].statespace.c.data (alpha) | [controllers.linear_controller[:].statespace.state_names, | FLT_3D (uncertain) | mixed | C matrix |
controllers.linear_controller[:].statespace.c.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].statespace.d (alpha) | STRUCTURE | D matrix, normally proper and D=0 | ||
controllers.linear_controller[:].statespace.d.data (alpha) | [controllers.linear_controller[:].statespace.input_names, | FLT_3D (uncertain) | mixed | D matrix, normally proper and D=0 |
controllers.linear_controller[:].statespace.d.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].statespace.deltat (alpha) | STRUCTURE | Discrete time sampling interval ; if less than 1e-10, the controller is considered to be expressed in continuous time | ||
controllers.linear_controller[:].statespace.deltat.data (alpha) | [controllers.linear_controller[:].statespace.deltat.time] | FLT_1D (uncertain) | s | Discrete time sampling interval ; if less than 1e-10, the controller is considered to be expressed in continuous time |
controllers.linear_controller[:].statespace.deltat.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.linear_controller[:].statespace.state_names (alpha) | [1...N] | STR_1D | Names of the states | |
controllers.nonlinear_controller (alpha) | [1...N] | STRUCT_ARRAY | A non-linear controller, this is less conventional and will have to be developed | |
controllers.nonlinear_controller[:].controller_class (alpha) | STR_0D | One of a known class of controllers | ||
controllers.nonlinear_controller[:].description (alpha) | STR_0D | Description of this controller | ||
controllers.nonlinear_controller[:].function (alpha) | STR_0D | Method to be defined | ||
controllers.nonlinear_controller[:].input_names (alpha) | [1...N] | STR_1D | Names of the input signals, following the SDN convention | |
controllers.nonlinear_controller[:].inputs (alpha) | STRUCTURE | Input signals; the timebase is common to inputs and outputs for any particular controller | ||
controllers.nonlinear_controller[:].inputs.data (alpha) | [controllers.nonlinear_controller[:].input_names, | FLT_2D (uncertain) | mixed | Input signals; the timebase is common to inputs and outputs for any particular controller |
controllers.nonlinear_controller[:].inputs.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.nonlinear_controller[:].name (alpha) | STR_0D | Name of this controller | ||
controllers.nonlinear_controller[:].output_names (alpha) | [1...N] | STR_1D | Output signal names following the SDN convention | |
controllers.nonlinear_controller[:].outputs (alpha) | STRUCTURE | Output signals; the timebase is common to inputs and outputs for any particular controller | ||
controllers.nonlinear_controller[:].outputs.data (alpha) | [controllers.nonlinear_controller[:].output_names, | FLT_2D (uncertain) | mixed | Output signals; the timebase is common to inputs and outputs for any particular controller |
controllers.nonlinear_controller[:].outputs.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
controllers.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
core_instant_changes | Instant changes of the radial core plasma profiles due to pellet, MHD, ... | |||
core_instant_changes.change | [1...N] | STRUCT_ARRAY | Set of instant change terms (each being due to a different phenomenon) | |
core_instant_changes.change[:].identifier | STRUCTURE | Instant change term identifier | ||
core_instant_changes.change[:].identifier.description | STR_0D | Verbose description | ||
core_instant_changes.change[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list) | ||
core_instant_changes.change[:].identifier.name | STR_0D | Short string identifier | ||
core_instant_changes.change[:].profiles_1d | [core_instant_changes.change[:].profiles_1d[:].time] | STRUCT_ARRAY | Changes in 1D core profiles for various time slices. This structure mirrors core_profiles/profiles_1d and describes instant changes to each of these physical quantities (i.e. a signed difference quantity after change - quantity before change) | |
core_instant_changes.change[:].profiles_1d[:].conductivity_parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | ohm^-1.m^-1 | Parallel conductivity |
core_instant_changes.change[:].profiles_1d[:].e_field | STRUCTURE | V.m^-1 | Electric field, averaged on the magnetic surface. E.g for the parellel component, average(E.B) / B0, using core_profiles/vacuum_toroidal_field/b0 | |
core_instant_changes.change[:].profiles_1d[:].e_field.diamagnetic | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Diamagnetic component |
core_instant_changes.change[:].profiles_1d[:].e_field.parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Parallel component |
core_instant_changes.change[:].profiles_1d[:].e_field.poloidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Poloidal component |
core_instant_changes.change[:].profiles_1d[:].e_field.radial | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Radial component |
core_instant_changes.change[:].profiles_1d[:].e_field.toroidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Toroidal component |
core_instant_changes.change[:].profiles_1d[:].e_field_parallel (obsolescent) | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Parallel electric field = average(E.B) / B0, where Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_instant_changes.change[:].profiles_1d[:].electrons | STRUCTURE | Quantities related to the electrons | ||
core_instant_changes.change[:].profiles_1d[:].electrons.density | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
core_instant_changes.change[:].profiles_1d[:].electrons.density_fast | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
core_instant_changes.change[:].profiles_1d[:].electrons.pressure | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
core_instant_changes.change[:].profiles_1d[:].electrons.pressure_fast_parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
core_instant_changes.change[:].profiles_1d[:].electrons.pressure_fast_perpendicular | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
core_instant_changes.change[:].profiles_1d[:].electrons.temperature | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
core_instant_changes.change[:].profiles_1d[:].electrons.velocity | STRUCTURE | m.s^-1 | Velocity | |
core_instant_changes.change[:].profiles_1d[:].electrons.velocity.diamagnetic | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_instant_changes.change[:].profiles_1d[:].electrons.velocity.parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_instant_changes.change[:].profiles_1d[:].electrons.velocity.poloidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_instant_changes.change[:].profiles_1d[:].electrons.velocity.radial | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_instant_changes.change[:].profiles_1d[:].electrons.velocity.toroidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_instant_changes.change[:].profiles_1d[:].electrons.velocity_pol (obsolescent) | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
core_instant_changes.change[:].profiles_1d[:].electrons.velocity_tor (obsolescent) | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
core_instant_changes.change[:].profiles_1d[:].grid | STRUCTURE | Radial grid | ||
core_instant_changes.change[:].profiles_1d[:].grid.area | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
core_instant_changes.change[:].profiles_1d[:].grid.psi | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
core_instant_changes.change[:].profiles_1d[:].grid.rho_tor | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
core_instant_changes.change[:].profiles_1d[:].grid.volume | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
core_instant_changes.change[:].profiles_1d[:].ion | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
core_instant_changes.change[:].profiles_1d[:].ion[:].density | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].ion[:].density_fast | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].ion[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
core_instant_changes.change[:].profiles_1d[:].ion[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
core_instant_changes.change[:].profiles_1d[:].ion[:].element[:].multiplicity | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
core_instant_changes.change[:].profiles_1d[:].ion[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
core_instant_changes.change[:].profiles_1d[:].ion[:].label | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
core_instant_changes.change[:].profiles_1d[:].ion[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
core_instant_changes.change[:].profiles_1d[:].ion[:].neutral_index | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
core_instant_changes.change[:].profiles_1d[:].ion[:].pressure | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].ion[:].pressure_fast_parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].ion[:].pressure_fast_perpendicular | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].ion[:].state | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].density | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].density_fast | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].ionisation_potential | FLT_0D (uncertain) | Elementary Charge Unit | Cumulative and average ionisation potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z'=0 to z-1)), where Epot is the ionisation potential of ion Xz’+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].label | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].pressure | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].pressure_fast_parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].pressure_fast_perpendicular | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].temperature | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].velocity | STRUCTURE | m.s^-1 | Velocity | |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].velocity.diamagnetic | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].velocity.parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].velocity.poloidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].velocity.radial | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].velocity.toroidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].z_average | FLT_0D (uncertain) | Elementary Charge Unit | Average Z of the charge state bundle (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].z_max | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].z_min | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
core_instant_changes.change[:].profiles_1d[:].ion[:].state[:].z_square_average | FLT_0D (uncertain) | Elementary Charge Unit | Average Z square of the charge state bundle (equal to z_min if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
core_instant_changes.change[:].profiles_1d[:].ion[:].temperature | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].ion[:].velocity | STRUCTURE | m.s^-1 | Velocity (average over charge states when multiple charge states are considered) | |
core_instant_changes.change[:].profiles_1d[:].ion[:].velocity.diamagnetic | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_instant_changes.change[:].profiles_1d[:].ion[:].velocity.parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_instant_changes.change[:].profiles_1d[:].ion[:].velocity.poloidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_instant_changes.change[:].profiles_1d[:].ion[:].velocity.radial | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_instant_changes.change[:].profiles_1d[:].ion[:].velocity.toroidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_instant_changes.change[:].profiles_1d[:].ion[:].velocity_pol (obsolescent) | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity (average over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].ion[:].velocity_tor (obsolescent) | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity (average over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].ion[:].z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed), volume averaged over plasma radius | |
core_instant_changes.change[:].profiles_1d[:].ion[:].z_ion_1d | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Average charge of the ion species (sum of states charge weighted by state density and divided by ion density) |
core_instant_changes.change[:].profiles_1d[:].ion[:].z_ion_square_1d | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Average sqare charge of the ion species (sum of states square charge weighted by state density and divided by ion density) |
core_instant_changes.change[:].profiles_1d[:].j_bootstrap | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Bootstrap current density = average(J_Bootstrap.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_instant_changes.change[:].profiles_1d[:].j_non_inductive | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Non-inductive (includes bootstrap) parallel current density = average(jni.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_instant_changes.change[:].profiles_1d[:].j_ohmic | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Ohmic parallel current density = average(J_Ohmic.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_instant_changes.change[:].profiles_1d[:].j_tor | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Total toroidal current density = average(J_Tor/R) / average(1/R) |
core_instant_changes.change[:].profiles_1d[:].j_total | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Total parallel current density = average(jtot.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_instant_changes.change[:].profiles_1d[:].magnetic_shear | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor |
core_instant_changes.change[:].profiles_1d[:].momentum_tor | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | kg.m^-1.s^-1 | Total plasma toroidal momentum, summed over ion species and electrons weighted by their density and major radius, i.e. sum_over_species(n*R*m*Vphi) |
core_instant_changes.change[:].profiles_1d[:].n_i_total_over_n_e | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal) |
core_instant_changes.change[:].profiles_1d[:].neutral | [1...N] | STRUCT_ARRAY | Quantities related to the different neutral species | |
core_instant_changes.change[:].profiles_1d[:].neutral[:].density | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].neutral[:].density_fast | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].neutral[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
core_instant_changes.change[:].profiles_1d[:].neutral[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
core_instant_changes.change[:].profiles_1d[:].neutral[:].element[:].multiplicity | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
core_instant_changes.change[:].profiles_1d[:].neutral[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
core_instant_changes.change[:].profiles_1d[:].neutral[:].ion_index | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].label | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].pressure | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].neutral[:].pressure_fast_parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].neutral[:].pressure_fast_perpendicular | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (energy, excitation, ...) | |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].density | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].density_fast | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].label | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].neutral_type | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].neutral_type.description | STR_0D | Verbose description | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].neutral_type.index | INT_0D | Integer identifier (enumeration index within a list) | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].neutral_type.name | STR_0D | Short string identifier | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].pressure | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].pressure_fast_parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].pressure_fast_perpendicular | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].temperature | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].velocity | STRUCTURE | m.s^-1 | Velocity | |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].velocity.diamagnetic | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].velocity.parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].velocity.poloidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].velocity.radial | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].velocity.toroidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
core_instant_changes.change[:].profiles_1d[:].neutral[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
core_instant_changes.change[:].profiles_1d[:].neutral[:].temperature | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
core_instant_changes.change[:].profiles_1d[:].neutral[:].velocity | STRUCTURE | m.s^-1 | Velocity (average over charge states when multiple charge states are considered) | |
core_instant_changes.change[:].profiles_1d[:].neutral[:].velocity.diamagnetic | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_instant_changes.change[:].profiles_1d[:].neutral[:].velocity.parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_instant_changes.change[:].profiles_1d[:].neutral[:].velocity.poloidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_instant_changes.change[:].profiles_1d[:].neutral[:].velocity.radial | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_instant_changes.change[:].profiles_1d[:].neutral[:].velocity.toroidal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_instant_changes.change[:].profiles_1d[:].pressure_ion_total | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total (sum over ion species) thermal ion pressure |
core_instant_changes.change[:].profiles_1d[:].pressure_parallel | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total parallel pressure (electrons+ions, thermal+non-thermal) |
core_instant_changes.change[:].profiles_1d[:].pressure_perpendicular | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total perpendicular pressure (electrons+ions, thermal+non-thermal) |
core_instant_changes.change[:].profiles_1d[:].pressure_thermal | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Thermal pressure (electrons+ions) |
core_instant_changes.change[:].profiles_1d[:].q | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Safety factor |
core_instant_changes.change[:].profiles_1d[:].t_i_average | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Ion temperature (averaged on charge states and ion species) |
core_instant_changes.change[:].profiles_1d[:].time | FLT_0D | s | Time | |
core_instant_changes.change[:].profiles_1d[:].zeff | [core_instant_changes.change[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Effective charge |
core_instant_changes.code | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
core_instant_changes.code.commit | STR_0D | Unique commit reference of software | ||
core_instant_changes.code.name | STR_0D | Name of software generating IDS | ||
core_instant_changes.code.output_flag | [core_instant_changes.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
core_instant_changes.code.parameters | STR_0D | List of the code specific parameters in XML format | ||
core_instant_changes.code.repository | STR_0D | URL of software repository | ||
core_instant_changes.code.version | STR_0D | Unique version (tag) of software | ||
core_instant_changes.ids_properties | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
core_instant_changes.ids_properties.comment | STR_0D | Any comment describing the content of this IDS | ||
core_instant_changes.ids_properties.homogeneous_time | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
core_instant_changes.ids_properties.occurrence | INT_0D | |||
core_instant_changes.time | [1...N] | FLT_1D_TYPE | Generic time [s] | |
core_instant_changes.vacuum_toroidal_field | STRUCTURE | Characteristics of the vacuum toroidal field (used in Rho_Tor definition and in the normalization of current densities) | ||
core_instant_changes.vacuum_toroidal_field.b0 | [core_instant_changes.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
core_instant_changes.vacuum_toroidal_field.r0 | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
core_profiles | Core plasma radial profiles | |||
core_profiles.code | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
core_profiles.code.commit | STR_0D | Unique commit reference of software | ||
core_profiles.code.name | STR_0D | Name of software generating IDS | ||
core_profiles.code.output_flag | [core_profiles.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
core_profiles.code.parameters | STR_0D | List of the code specific parameters in XML format | ||
core_profiles.code.repository | STR_0D | URL of software repository | ||
core_profiles.code.version | STR_0D | Unique version (tag) of software | ||
core_profiles.global_quantities | STRUCTURE | Various global quantities derived from the profiles | ||
core_profiles.global_quantities.beta_pol | [core_profiles.time] | FLT_1D (uncertain) | - | Poloidal beta. Defined as betap = 4 int(p dV) / [R_0 * mu_0 * Ip^2] |
core_profiles.global_quantities.beta_tor | [core_profiles.time] | FLT_1D (uncertain) | - | Toroidal beta, defined as the volume-averaged total perpendicular pressure divided by (B0^2/(2*mu0)), i.e. beta_toroidal = 2 mu0 int(p dV) / V / B0^2 |
core_profiles.global_quantities.beta_tor_norm | [core_profiles.time] | FLT_1D (uncertain) | - | Normalised toroidal beta, defined as 100 * beta_tor * a[m] * B0 [T] / ip [MA] |
core_profiles.global_quantities.current_bootstrap | [core_profiles.time] | FLT_1D (uncertain) | A | Bootstrap current |
core_profiles.global_quantities.current_non_inductive | [core_profiles.time] | FLT_1D (uncertain) | A | Total non-inductive parallel current |
core_profiles.global_quantities.energy_diamagnetic | [core_profiles.time] | FLT_1D (uncertain) | J | Plasma energy content = 3/2 * integral over the plasma volume of the total perpendicular pressure |
core_profiles.global_quantities.ip | [core_profiles.time] | FLT_1D (uncertain) | A | Total plasma current |
core_profiles.global_quantities.li (obsolescent) | [core_profiles.time] | FLT_1D (uncertain) | - | Internal inductance. The li_3 definition is used, i.e. li_3 = 2/R0/mu0^2/Ip^2 * int(Bp^2 dV). |
core_profiles.global_quantities.li_3 | [core_profiles.time] | FLT_1D (uncertain) | - | Internal inductance. The li_3 definition is used, i.e. li_3 = 2/R0/mu0^2/Ip^2 * int(Bp^2 dV). |
core_profiles.global_quantities.v_loop | [core_profiles.time] | FLT_1D (uncertain) | V | LCFS loop voltage |
core_profiles.ids_properties | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
core_profiles.ids_properties.comment | STR_0D | Any comment describing the content of this IDS | ||
core_profiles.ids_properties.homogeneous_time | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
core_profiles.ids_properties.occurrence | INT_0D | |||
core_profiles.profiles_1d | [core_profiles.profiles_1d[:].time] | STRUCT_ARRAY | Core plasma radial profiles for various time slices | |
core_profiles.profiles_1d[:].conductivity_parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | ohm^-1.m^-1 | Parallel conductivity |
core_profiles.profiles_1d[:].e_field | STRUCTURE | V.m^-1 | Electric field, averaged on the magnetic surface. E.g for the parellel component, average(E.B) / B0, using core_profiles/vacuum_toroidal_field/b0 | |
core_profiles.profiles_1d[:].e_field.diamagnetic | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Diamagnetic component |
core_profiles.profiles_1d[:].e_field.parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Parallel component |
core_profiles.profiles_1d[:].e_field.poloidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Poloidal component |
core_profiles.profiles_1d[:].e_field.radial | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Radial component |
core_profiles.profiles_1d[:].e_field.toroidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Toroidal component |
core_profiles.profiles_1d[:].e_field_parallel (obsolescent) | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Parallel electric field = average(E.B) / B0, where Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_profiles.profiles_1d[:].electrons | STRUCTURE | Quantities related to the electrons | ||
core_profiles.profiles_1d[:].electrons.density | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
core_profiles.profiles_1d[:].electrons.density_fast | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
core_profiles.profiles_1d[:].electrons.pressure | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
core_profiles.profiles_1d[:].electrons.pressure_fast_parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
core_profiles.profiles_1d[:].electrons.pressure_fast_perpendicular | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
core_profiles.profiles_1d[:].electrons.temperature | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
core_profiles.profiles_1d[:].electrons.velocity | STRUCTURE | m.s^-1 | Velocity | |
core_profiles.profiles_1d[:].electrons.velocity.diamagnetic | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_profiles.profiles_1d[:].electrons.velocity.parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_profiles.profiles_1d[:].electrons.velocity.poloidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_profiles.profiles_1d[:].electrons.velocity.radial | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_profiles.profiles_1d[:].electrons.velocity.toroidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_profiles.profiles_1d[:].electrons.velocity_pol (obsolescent) | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
core_profiles.profiles_1d[:].electrons.velocity_tor (obsolescent) | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
core_profiles.profiles_1d[:].grid | STRUCTURE | Radial grid | ||
core_profiles.profiles_1d[:].grid.area | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
core_profiles.profiles_1d[:].grid.psi | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
core_profiles.profiles_1d[:].grid.rho_tor | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
core_profiles.profiles_1d[:].grid.rho_tor_norm | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
core_profiles.profiles_1d[:].grid.volume | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
core_profiles.profiles_1d[:].ion | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
core_profiles.profiles_1d[:].ion[:].density | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].ion[:].density_fast | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].ion[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
core_profiles.profiles_1d[:].ion[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
core_profiles.profiles_1d[:].ion[:].element[:].multiplicity | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
core_profiles.profiles_1d[:].ion[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
core_profiles.profiles_1d[:].ion[:].label | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
core_profiles.profiles_1d[:].ion[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
core_profiles.profiles_1d[:].ion[:].neutral_index | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
core_profiles.profiles_1d[:].ion[:].pressure | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].ion[:].pressure_fast_parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].ion[:].pressure_fast_perpendicular | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].ion[:].state | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
core_profiles.profiles_1d[:].ion[:].state[:].density | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
core_profiles.profiles_1d[:].ion[:].state[:].density_fast | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
core_profiles.profiles_1d[:].ion[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
core_profiles.profiles_1d[:].ion[:].state[:].ionisation_potential | FLT_0D (uncertain) | Elementary Charge Unit | Cumulative and average ionisation potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z'=0 to z-1)), where Epot is the ionisation potential of ion Xz’+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
core_profiles.profiles_1d[:].ion[:].state[:].label | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
core_profiles.profiles_1d[:].ion[:].state[:].pressure | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
core_profiles.profiles_1d[:].ion[:].state[:].pressure_fast_parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
core_profiles.profiles_1d[:].ion[:].state[:].pressure_fast_perpendicular | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
core_profiles.profiles_1d[:].ion[:].state[:].temperature | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
core_profiles.profiles_1d[:].ion[:].state[:].velocity | STRUCTURE | m.s^-1 | Velocity | |
core_profiles.profiles_1d[:].ion[:].state[:].velocity.diamagnetic | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_profiles.profiles_1d[:].ion[:].state[:].velocity.parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_profiles.profiles_1d[:].ion[:].state[:].velocity.poloidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_profiles.profiles_1d[:].ion[:].state[:].velocity.radial | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_profiles.profiles_1d[:].ion[:].state[:].velocity.toroidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_profiles.profiles_1d[:].ion[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
core_profiles.profiles_1d[:].ion[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
core_profiles.profiles_1d[:].ion[:].state[:].z_average | FLT_0D (uncertain) | Elementary Charge Unit | Average Z of the charge state bundle (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
core_profiles.profiles_1d[:].ion[:].state[:].z_max | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
core_profiles.profiles_1d[:].ion[:].state[:].z_min | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
core_profiles.profiles_1d[:].ion[:].state[:].z_square_average | FLT_0D (uncertain) | Elementary Charge Unit | Average Z square of the charge state bundle (equal to z_min if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
core_profiles.profiles_1d[:].ion[:].temperature | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].ion[:].velocity | STRUCTURE | m.s^-1 | Velocity (average over charge states when multiple charge states are considered) | |
core_profiles.profiles_1d[:].ion[:].velocity.diamagnetic | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_profiles.profiles_1d[:].ion[:].velocity.parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_profiles.profiles_1d[:].ion[:].velocity.poloidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_profiles.profiles_1d[:].ion[:].velocity.radial | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_profiles.profiles_1d[:].ion[:].velocity.toroidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_profiles.profiles_1d[:].ion[:].velocity_pol (obsolescent) | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity (average over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].ion[:].velocity_tor (obsolescent) | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity (average over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].ion[:].z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed), volume averaged over plasma radius | |
core_profiles.profiles_1d[:].ion[:].z_ion_1d | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Average charge of the ion species (sum of states charge weighted by state density and divided by ion density) |
core_profiles.profiles_1d[:].ion[:].z_ion_square_1d | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Average sqare charge of the ion species (sum of states square charge weighted by state density and divided by ion density) |
core_profiles.profiles_1d[:].j_bootstrap | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Bootstrap current density = average(J_Bootstrap.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_profiles.profiles_1d[:].j_non_inductive | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Non-inductive (includes bootstrap) parallel current density = average(jni.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_profiles.profiles_1d[:].j_ohmic | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Ohmic parallel current density = average(J_Ohmic.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_profiles.profiles_1d[:].j_tor | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Total toroidal current density = average(J_Tor/R) / average(1/R) |
core_profiles.profiles_1d[:].j_total | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Total parallel current density = average(jtot.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
core_profiles.profiles_1d[:].magnetic_shear | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor |
core_profiles.profiles_1d[:].momentum_tor | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | kg.m^-1.s^-1 | Total plasma toroidal momentum, summed over ion species and electrons weighted by their density and major radius, i.e. sum_over_species(n*R*m*Vphi) |
core_profiles.profiles_1d[:].n_i_total_over_n_e | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal) |
core_profiles.profiles_1d[:].neutral | [1...N] | STRUCT_ARRAY | Quantities related to the different neutral species | |
core_profiles.profiles_1d[:].neutral[:].density | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].neutral[:].density_fast | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].neutral[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
core_profiles.profiles_1d[:].neutral[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
core_profiles.profiles_1d[:].neutral[:].element[:].multiplicity | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
core_profiles.profiles_1d[:].neutral[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
core_profiles.profiles_1d[:].neutral[:].ion_index | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
core_profiles.profiles_1d[:].neutral[:].label | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
core_profiles.profiles_1d[:].neutral[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
core_profiles.profiles_1d[:].neutral[:].pressure | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].neutral[:].pressure_fast_parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].neutral[:].pressure_fast_perpendicular | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].neutral[:].state | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (energy, excitation, ...) | |
core_profiles.profiles_1d[:].neutral[:].state[:].density | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
core_profiles.profiles_1d[:].neutral[:].state[:].density_fast | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
core_profiles.profiles_1d[:].neutral[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
core_profiles.profiles_1d[:].neutral[:].state[:].label | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
core_profiles.profiles_1d[:].neutral[:].state[:].neutral_type | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
core_profiles.profiles_1d[:].neutral[:].state[:].neutral_type.description | STR_0D | Verbose description | ||
core_profiles.profiles_1d[:].neutral[:].state[:].neutral_type.index | INT_0D | Integer identifier (enumeration index within a list) | ||
core_profiles.profiles_1d[:].neutral[:].state[:].neutral_type.name | STR_0D | Short string identifier | ||
core_profiles.profiles_1d[:].neutral[:].state[:].pressure | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
core_profiles.profiles_1d[:].neutral[:].state[:].pressure_fast_parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
core_profiles.profiles_1d[:].neutral[:].state[:].pressure_fast_perpendicular | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
core_profiles.profiles_1d[:].neutral[:].state[:].temperature | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
core_profiles.profiles_1d[:].neutral[:].state[:].velocity | STRUCTURE | m.s^-1 | Velocity | |
core_profiles.profiles_1d[:].neutral[:].state[:].velocity.diamagnetic | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_profiles.profiles_1d[:].neutral[:].state[:].velocity.parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_profiles.profiles_1d[:].neutral[:].state[:].velocity.poloidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_profiles.profiles_1d[:].neutral[:].state[:].velocity.radial | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_profiles.profiles_1d[:].neutral[:].state[:].velocity.toroidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_profiles.profiles_1d[:].neutral[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
core_profiles.profiles_1d[:].neutral[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
core_profiles.profiles_1d[:].neutral[:].temperature | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
core_profiles.profiles_1d[:].neutral[:].velocity | STRUCTURE | m.s^-1 | Velocity (average over charge states when multiple charge states are considered) | |
core_profiles.profiles_1d[:].neutral[:].velocity.diamagnetic | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
core_profiles.profiles_1d[:].neutral[:].velocity.parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
core_profiles.profiles_1d[:].neutral[:].velocity.poloidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
core_profiles.profiles_1d[:].neutral[:].velocity.radial | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
core_profiles.profiles_1d[:].neutral[:].velocity.toroidal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
core_profiles.profiles_1d[:].pressure_ion_total | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total (sum over ion species) thermal ion pressure |
core_profiles.profiles_1d[:].pressure_parallel | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total parallel pressure (electrons+ions, thermal+non-thermal) |
core_profiles.profiles_1d[:].pressure_perpendicular | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total perpendicular pressure (electrons+ions, thermal+non-thermal) |
core_profiles.profiles_1d[:].pressure_thermal | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Thermal pressure (electrons+ions) |
core_profiles.profiles_1d[:].q | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Safety factor |
core_profiles.profiles_1d[:].t_i_average | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Ion temperature (averaged on charge states and ion species) |
core_profiles.profiles_1d[:].time | FLT_0D | s | Time | |
core_profiles.profiles_1d[:].zeff | [core_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Effective charge |
core_profiles.time | [1...N] | FLT_1D_TYPE | Generic time [s] | |
core_profiles.vacuum_toroidal_field | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities) | ||
core_profiles.vacuum_toroidal_field.b0 | [core_profiles.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
core_profiles.vacuum_toroidal_field.r0 | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
core_sources | Core plasma source terms (for the transport equations). Energy terms correspond to the full kinetic energy equation (i.e. the energy flux takes into account the energy transported by the particle flux) | |||
core_sources.code | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
core_sources.code.commit | STR_0D | Unique commit reference of software | ||
core_sources.code.name | STR_0D | Name of software generating IDS | ||
core_sources.code.output_flag | [core_sources.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
core_sources.code.parameters | STR_0D | List of the code specific parameters in XML format | ||
core_sources.code.repository | STR_0D | URL of software repository | ||
core_sources.code.version | STR_0D | Unique version (tag) of software | ||
core_sources.ids_properties | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
core_sources.ids_properties.comment | STR_0D | Any comment describing the content of this IDS | ||
core_sources.ids_properties.homogeneous_time | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
core_sources.ids_properties.occurrence | INT_0D | |||
core_sources.source | [1...N] | STRUCT_ARRAY | Set of source terms | |
core_sources.source[:].global_quantities | [core_sources.source[:].global_quantities[:].time] | STRUCT_ARRAY | Total source quantities integrated over the plasma volume or surface | |
core_sources.source[:].global_quantities[:].current_parallel | FLT_0D (uncertain) | A.m | Parallel current driven | |
core_sources.source[:].global_quantities[:].electrons | STRUCTURE | Sources for electrons | ||
core_sources.source[:].global_quantities[:].electrons.particles | FLT_0D (uncertain) | s^-1 | Electron particle source | |
core_sources.source[:].global_quantities[:].electrons.power | FLT_0D (uncertain) | W | Power coupled to electrons | |
core_sources.source[:].global_quantities[:].power | FLT_0D (uncertain) | W | Total power coupled to the plasma | |
core_sources.source[:].global_quantities[:].time | FLT_0D | s | Time | |
core_sources.source[:].global_quantities[:].torque_tor | FLT_0D (uncertain) | kg.m^2.s^-2 | Toroidal torque | |
core_sources.source[:].global_quantities[:].total_ion_power | FLT_0D (uncertain) | W | Total power coupled to ion species (summed over ion species) | |
core_sources.source[:].identifier | STRUCTURE | Source term identifier | ||
core_sources.source[:].identifier.description | STR_0D | Verbose description | ||
core_sources.source[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list) | ||
core_sources.source[:].identifier.name | STR_0D | Short string identifier | ||
core_sources.source[:].profiles_1d | [core_sources.source[:].profiles_1d[:].time] | STRUCT_ARRAY | Source profiles for various time slices. Source terms are positive (resp. negative) when there is a gain (resp. a loss) to the considered channel. | |
core_sources.source[:].profiles_1d[:].conductivity_parallel | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | ohm^-1.m^-1 | Parallel conductivity due to this source |
core_sources.source[:].profiles_1d[:].current_parallel_inside | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A | Parallel current driven inside the flux surface. Cumulative surface integral of j_parallel |
core_sources.source[:].profiles_1d[:].electrons | STRUCTURE | Sources for electrons | ||
core_sources.source[:].profiles_1d[:].electrons.energy | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source term for the electron energy equation |
core_sources.source[:].profiles_1d[:].electrons.particles | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3.s^-1 | Source term for electron density equation |
core_sources.source[:].profiles_1d[:].electrons.particles_inside | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1 | Electron source inside the flux surface. Cumulative volume integral of the source term for the electron density equation. |
core_sources.source[:].profiles_1d[:].electrons.power_inside | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W | Power coupled to electrons inside the flux surface. Cumulative volume integral of the source term for the electron energy equation |
core_sources.source[:].profiles_1d[:].grid | STRUCTURE | Radial grid | ||
core_sources.source[:].profiles_1d[:].grid.area | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
core_sources.source[:].profiles_1d[:].grid.psi | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
core_sources.source[:].profiles_1d[:].grid.rho_tor | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
core_sources.source[:].profiles_1d[:].grid.rho_tor_norm | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
core_sources.source[:].profiles_1d[:].grid.volume | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
core_sources.source[:].profiles_1d[:].ion | [1...N] | STRUCT_ARRAY | Source terms related to the different ions species | |
core_sources.source[:].profiles_1d[:].ion[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
core_sources.source[:].profiles_1d[:].ion[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
core_sources.source[:].profiles_1d[:].ion[:].element[:].multiplicity | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
core_sources.source[:].profiles_1d[:].ion[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
core_sources.source[:].profiles_1d[:].ion[:].energy | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source term for the ion energy transport equation. |
core_sources.source[:].profiles_1d[:].ion[:].label | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
core_sources.source[:].profiles_1d[:].ion[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
core_sources.source[:].profiles_1d[:].ion[:].neutral_index | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
core_sources.source[:].profiles_1d[:].ion[:].particles | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source term for ion density equation |
core_sources.source[:].profiles_1d[:].ion[:].state | [1...N] | STRUCT_ARRAY | Source terms related to the different charge states of the species (ionisation, energy, excitation, ...) | |
core_sources.source[:].profiles_1d[:].ion[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
core_sources.source[:].profiles_1d[:].ion[:].state[:].energy | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source terms for the charge state energy transport equation |
core_sources.source[:].profiles_1d[:].ion[:].state[:].is_neutral (obsolescent) | INT_0D | Flag specifying if this state corresponds to a neutral (1) or not (0) | ||
core_sources.source[:].profiles_1d[:].ion[:].state[:].label | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
core_sources.source[:].profiles_1d[:].ion[:].state[:].neutral_type (obsolescent) | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
core_sources.source[:].profiles_1d[:].ion[:].state[:].neutral_type.description (obsolescent) | STR_0D | Verbose description | ||
core_sources.source[:].profiles_1d[:].ion[:].state[:].neutral_type.index (obsolescent) | INT_0D | Integer identifier (enumeration index within a list) | ||
core_sources.source[:].profiles_1d[:].ion[:].state[:].neutral_type.name (obsolescent) | STR_0D | Short string identifier | ||
core_sources.source[:].profiles_1d[:].ion[:].state[:].particles | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source term for the charge state density transport equation |
core_sources.source[:].profiles_1d[:].ion[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
core_sources.source[:].profiles_1d[:].ion[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
core_sources.source[:].profiles_1d[:].ion[:].state[:].z_max | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle | |
core_sources.source[:].profiles_1d[:].ion[:].state[:].z_min | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
core_sources.source[:].profiles_1d[:].ion[:].z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
core_sources.source[:].profiles_1d[:].j_parallel | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Parallel current density source, average(J.B) / B0, where B0 = core_sources/vacuum_toroidal_field/b0 |
core_sources.source[:].profiles_1d[:].momentum_tor | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Source term for total toroidal momentum equation |
core_sources.source[:].profiles_1d[:].neutral | [1...N] | STRUCT_ARRAY | Source terms related to the different neutral species | |
core_sources.source[:].profiles_1d[:].neutral[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
core_sources.source[:].profiles_1d[:].neutral[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
core_sources.source[:].profiles_1d[:].neutral[:].element[:].multiplicity | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
core_sources.source[:].profiles_1d[:].neutral[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
core_sources.source[:].profiles_1d[:].neutral[:].energy | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source term for the ion energy transport equation. |
core_sources.source[:].profiles_1d[:].neutral[:].ion_index | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
core_sources.source[:].profiles_1d[:].neutral[:].label | STR_0D | String identifying the neutral species (e.g. H, D, T, He, C, ...) | ||
core_sources.source[:].profiles_1d[:].neutral[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
core_sources.source[:].profiles_1d[:].neutral[:].particles | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source term for ion density equation |
core_sources.source[:].profiles_1d[:].neutral[:].state | [1...N] | STRUCT_ARRAY | Source terms related to the different charge states of the species (energy, excitation, ...) | |
core_sources.source[:].profiles_1d[:].neutral[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
core_sources.source[:].profiles_1d[:].neutral[:].state[:].energy | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source terms for the charge state energy transport equation |
core_sources.source[:].profiles_1d[:].neutral[:].state[:].label | STR_0D | String identifying state | ||
core_sources.source[:].profiles_1d[:].neutral[:].state[:].neutral_type | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
core_sources.source[:].profiles_1d[:].neutral[:].state[:].neutral_type.description | STR_0D | Verbose description | ||
core_sources.source[:].profiles_1d[:].neutral[:].state[:].neutral_type.index | INT_0D | Integer identifier (enumeration index within a list) | ||
core_sources.source[:].profiles_1d[:].neutral[:].state[:].neutral_type.name | STR_0D | Short string identifier | ||
core_sources.source[:].profiles_1d[:].neutral[:].state[:].particles | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source term for the charge state density transport equation |
core_sources.source[:].profiles_1d[:].neutral[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
core_sources.source[:].profiles_1d[:].neutral[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
core_sources.source[:].profiles_1d[:].time | FLT_0D | s | Time | |
core_sources.source[:].profiles_1d[:].torque_tor_inside | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | kg.m^2.s^-2 | Toroidal torque inside the flux surface. Cumulative volume integral of the source term for the total toroidal momentum equation |
core_sources.source[:].profiles_1d[:].total_ion_energy | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source term for the total (summed over ion species) energy equation |
core_sources.source[:].profiles_1d[:].total_ion_power_inside | [core_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W | Total power coupled to ion species (summed over ion species) inside the flux surface. Cumulative volume integral of the source term for the total ion energy equation |
core_sources.time | [1...N] | FLT_1D_TYPE | Generic time [s] | |
core_sources.vacuum_toroidal_field | STRUCTURE | Characteristics of the vacuum toroidal field (used in Rho_Tor definition and in the normalization of current densities) | ||
core_sources.vacuum_toroidal_field.b0 | [core_sources.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
core_sources.vacuum_toroidal_field.r0 | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
core_transport | Core plasma transport. Energy terms correspond to the full kinetic energy equation (i.e. the energy flux takes into account the energy transported by the particle flux) | |||
core_transport.code | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
core_transport.code.commit | STR_0D | Unique commit reference of software | ||
core_transport.code.name | STR_0D | Name of software generating IDS | ||
core_transport.code.output_flag | [core_transport.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
core_transport.code.parameters | STR_0D | List of the code specific parameters in XML format | ||
core_transport.code.repository | STR_0D | URL of software repository | ||
core_transport.code.version | STR_0D | Unique version (tag) of software | ||
core_transport.ids_properties | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
core_transport.ids_properties.comment | STR_0D | Any comment describing the content of this IDS | ||
core_transport.ids_properties.homogeneous_time | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
core_transport.ids_properties.occurrence | INT_0D | |||
core_transport.model | [1...N_Models] | STRUCT_ARRAY | Transport is described by a combination of various transport models | |
core_transport.model[:].flux_multiplier | FLT_0D (uncertain) | - | Multiplier applied to the particule flux when adding its contribution in the expression of the heat flux : can be 0, 3/2 or 5/2 | |
core_transport.model[:].identifier | STRUCTURE | Transport model identifier | ||
core_transport.model[:].identifier.description | STR_0D | Verbose description | ||
core_transport.model[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list) | ||
core_transport.model[:].identifier.name | STR_0D | Short string identifier | ||
core_transport.model[:].profiles_1d | [core_transport.model[:].profiles_1d[:].time] | STRUCT_ARRAY | Transport coefficient profiles for various time slices. Fluxes and convection are positive (resp. negative) when outwards i.e. towards the LCFS (resp. inwards i.e. towards the magnetic axes). | |
core_transport.model[:].profiles_1d[:].conductivity_parallel | [core_transport.model[:].profiles_1d[:].rho_tor_norm] | FLT_1D (uncertain) | ohm^-1.m^-1 | Parallel conductivity |
core_transport.model[:].profiles_1d[:].electrons | STRUCTURE | Transport quantities related to the electrons | ||
core_transport.model[:].profiles_1d[:].electrons.energy | STRUCTURE | Transport quantities for the electron energy equation | ||
core_transport.model[:].profiles_1d[:].electrons.energy.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].electrons.energy.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | W.m^-2 | Flux |
core_transport.model[:].profiles_1d[:].electrons.energy.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].electrons.particles | STRUCTURE | Transport quantities for the electron density equation | ||
core_transport.model[:].profiles_1d[:].electrons.particles.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].electrons.particles.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | m^-2.s^-1 | Flux |
core_transport.model[:].profiles_1d[:].electrons.particles.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].grid_d | STRUCTURE | Grid for effective diffusivities and parallel conductivity | ||
core_transport.model[:].profiles_1d[:].grid_d.area | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
core_transport.model[:].profiles_1d[:].grid_d.psi | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
core_transport.model[:].profiles_1d[:].grid_d.rho_tor | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
core_transport.model[:].profiles_1d[:].grid_d.volume | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
core_transport.model[:].profiles_1d[:].grid_flux | STRUCTURE | Grid for fluxes | ||
core_transport.model[:].profiles_1d[:].grid_flux.area | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
core_transport.model[:].profiles_1d[:].grid_flux.psi | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
core_transport.model[:].profiles_1d[:].grid_flux.rho_tor | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
core_transport.model[:].profiles_1d[:].grid_flux.volume | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
core_transport.model[:].profiles_1d[:].grid_v | STRUCTURE | Grid for effective convections | ||
core_transport.model[:].profiles_1d[:].grid_v.area | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
core_transport.model[:].profiles_1d[:].grid_v.psi | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
core_transport.model[:].profiles_1d[:].grid_v.rho_tor | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
core_transport.model[:].profiles_1d[:].grid_v.volume | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
core_transport.model[:].profiles_1d[:].ion | [1...N] | STRUCT_ARRAY | Transport coefficients related to the various ion species | |
core_transport.model[:].profiles_1d[:].ion[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
core_transport.model[:].profiles_1d[:].ion[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
core_transport.model[:].profiles_1d[:].ion[:].element[:].multiplicity | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
core_transport.model[:].profiles_1d[:].ion[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
core_transport.model[:].profiles_1d[:].ion[:].energy | STRUCTURE | Transport coefficients related to the ion energy equation | ||
core_transport.model[:].profiles_1d[:].ion[:].energy.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].ion[:].energy.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | W.m^-2 | Flux |
core_transport.model[:].profiles_1d[:].ion[:].energy.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].ion[:].label | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
core_transport.model[:].profiles_1d[:].ion[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
core_transport.model[:].profiles_1d[:].ion[:].neutral_index | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
core_transport.model[:].profiles_1d[:].ion[:].particles | STRUCTURE | Transport related to the ion density equation | ||
core_transport.model[:].profiles_1d[:].ion[:].particles.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].ion[:].particles.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | m^-2.s^-1 | Flux |
core_transport.model[:].profiles_1d[:].ion[:].particles.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].ion[:].state | [1...N] | STRUCT_ARRAY | Transport coefficients related to the different states of the species | |
core_transport.model[:].profiles_1d[:].ion[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].energy | STRUCTURE | Transport quantities related to the energy equation of the charge state considered | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].energy.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].ion[:].state[:].energy.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | W.m^-2 | Flux |
core_transport.model[:].profiles_1d[:].ion[:].state[:].energy.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].ion[:].state[:].is_neutral (obsolescent) | INT_0D | Flag specifying if this state corresponds to a neutral (1) or not (0) | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].label | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].neutral_type (obsolescent) | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].neutral_type.description (obsolescent) | STR_0D | Verbose description | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].neutral_type.index (obsolescent) | INT_0D | Integer identifier (enumeration index within a list) | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].neutral_type.name (obsolescent) | STR_0D | Short string identifier | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].particles | STRUCTURE | Transport quantities related to density equation of the charge state considered (thermal+non-thermal) | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].particles.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].ion[:].state[:].particles.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | m^-2.s^-1 | Flux |
core_transport.model[:].profiles_1d[:].ion[:].state[:].particles.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].ion[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
core_transport.model[:].profiles_1d[:].ion[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
core_transport.model[:].profiles_1d[:].ion[:].state[:].z_max | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle | |
core_transport.model[:].profiles_1d[:].ion[:].state[:].z_min | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
core_transport.model[:].profiles_1d[:].ion[:].z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
core_transport.model[:].profiles_1d[:].momentum_tor | STRUCTURE | Transport coefficients for total toroidal momentum equation | ||
core_transport.model[:].profiles_1d[:].momentum_tor.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].momentum_tor.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Flux |
core_transport.model[:].profiles_1d[:].momentum_tor.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].neutral | [1...N] | STRUCT_ARRAY | Transport coefficients related to the various neutral species | |
core_transport.model[:].profiles_1d[:].neutral[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
core_transport.model[:].profiles_1d[:].neutral[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
core_transport.model[:].profiles_1d[:].neutral[:].element[:].multiplicity | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
core_transport.model[:].profiles_1d[:].neutral[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
core_transport.model[:].profiles_1d[:].neutral[:].energy | STRUCTURE | Transport coefficients related to the neutral energy equation | ||
core_transport.model[:].profiles_1d[:].neutral[:].energy.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].neutral[:].energy.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | W.m^-2 | Flux |
core_transport.model[:].profiles_1d[:].neutral[:].energy.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].neutral[:].ion_index | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
core_transport.model[:].profiles_1d[:].neutral[:].label | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
core_transport.model[:].profiles_1d[:].neutral[:].multiple_states_flag | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
core_transport.model[:].profiles_1d[:].neutral[:].particles | STRUCTURE | Transport related to the neutral density equation | ||
core_transport.model[:].profiles_1d[:].neutral[:].particles.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].neutral[:].particles.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | m^-2.s^-1 | Flux |
core_transport.model[:].profiles_1d[:].neutral[:].particles.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].neutral[:].state | [1...N] | STRUCT_ARRAY | Transport coefficients related to the different states of the species | |
core_transport.model[:].profiles_1d[:].neutral[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
core_transport.model[:].profiles_1d[:].neutral[:].state[:].energy | STRUCTURE | Transport quantities related to the energy equation of the charge state considered | ||
core_transport.model[:].profiles_1d[:].neutral[:].state[:].energy.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].neutral[:].state[:].energy.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | W.m^-2 | Flux |
core_transport.model[:].profiles_1d[:].neutral[:].state[:].energy.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].neutral[:].state[:].label | STR_0D | String identifying state | ||
core_transport.model[:].profiles_1d[:].neutral[:].state[:].particles | STRUCTURE | Transport quantities related to density equation of the charge state considered (thermal+non-thermal) | ||
core_transport.model[:].profiles_1d[:].neutral[:].state[:].particles.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].neutral[:].state[:].particles.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | m^-2.s^-1 | Flux |
core_transport.model[:].profiles_1d[:].neutral[:].state[:].particles.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.model[:].profiles_1d[:].neutral[:].state[:].vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
core_transport.model[:].profiles_1d[:].neutral[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
core_transport.model[:].profiles_1d[:].time | FLT_0D | s | Time | |
core_transport.model[:].profiles_1d[:].total_ion_energy | STRUCTURE | Transport coefficients for the total (summed over ion species) energy equation | ||
core_transport.model[:].profiles_1d[:].total_ion_energy.d | [core_transport.model[:].profiles_1d[:].grid_d.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Effective diffusivity |
core_transport.model[:].profiles_1d[:].total_ion_energy.flux | [core_transport.model[:].profiles_1d[:].grid_flux.rho_tor_norm] | FLT_1D (uncertain) | W.m^-2 | Flux |
core_transport.model[:].profiles_1d[:].total_ion_energy.v | [core_transport.model[:].profiles_1d[:].grid_v.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Effective convection |
core_transport.time | [1...N] | FLT_1D_TYPE | Generic time [s] | |
core_transport.vacuum_toroidal_field | STRUCTURE | Characteristics of the vacuum toroidal field (used in Rho_Tor definition and in the normalization of current densities) | ||
core_transport.vacuum_toroidal_field.b0 | [core_transport.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
core_transport.vacuum_toroidal_field.r0 | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
dataset_description (alpha) | General description of the dataset (collection of all IDSs within the given database entry). Main description text to be put in ids_properties/comment | |||
dataset_description.data_entry (alpha) | STRUCTURE | Definition of this data entry | ||
dataset_description.data_entry.machine (alpha) | STR_0D | Name of the experimental device to which this data is related | ||
dataset_description.data_entry.pulse (alpha) | INT_0D | Pulse number | ||
dataset_description.data_entry.pulse_type (alpha) | STR_0D | Type of the data entry, e.g. "pulse", "simulation", ... | ||
dataset_description.data_entry.run (alpha) | INT_0D | Run number | ||
dataset_description.data_entry.user (alpha) | STR_0D | Username | ||
dataset_description.dd_version (alpha) | STR_0D | Version of the physics data dictionary of this dataset | ||
dataset_description.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
dataset_description.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
dataset_description.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
dataset_description.ids_properties.occurrence | INT_0D | |||
dataset_description.imas_version (alpha) | STR_0D | Version of the IMAS infrastructure used to produce this data entry. Refers to the global IMAS repository which links to versions of every infrastructure tools | ||
dataset_description.parent_entry (alpha) | STRUCTURE | Definition of the parent data entry, if the present data entry has been generated by applying a given workflow to a unique parent entry | ||
dataset_description.parent_entry.machine (alpha) | STR_0D | Name of the experimental device to which this data is related | ||
dataset_description.parent_entry.pulse (alpha) | INT_0D | Pulse number | ||
dataset_description.parent_entry.pulse_type (alpha) | STR_0D | Type of the data entry, e.g. "pulse", "simulation", ... | ||
dataset_description.parent_entry.run (alpha) | INT_0D | Run number | ||
dataset_description.parent_entry.user (alpha) | STR_0D | Username | ||
dataset_description.simulation (alpha) | STRUCTURE | Description of the general simulation characteristics, if this data entry has been produced by a simulation. Several nodes describe typical time-dependent simulation with a time evolution as the main loop | ||
dataset_description.simulation.comment_after (alpha) | STR_0D | Comment made at the end of a simulation | ||
dataset_description.simulation.comment_before (alpha) | STR_0D | Comment made when launching a simulation | ||
dataset_description.simulation.time_begin (alpha) | FLT_0D (uncertain) | s | Start time | |
dataset_description.simulation.time_begun (alpha) | STR_0D | UTC | Actual wall-clock time simulation started | |
dataset_description.simulation.time_current (alpha) | FLT_0D (uncertain) | s | Current time of the simulation | |
dataset_description.simulation.time_end (alpha) | FLT_0D (uncertain) | s | Stop time | |
dataset_description.simulation.time_ended (alpha) | STR_0D | UTC | Actual wall-clock time simulation finished | |
dataset_description.simulation.time_restart (alpha) | FLT_0D (uncertain) | s | Time of the last restart done during the simulation | |
dataset_description.simulation.time_step (alpha) | FLT_0D (uncertain) | s | Time interval between main steps, e.g. storage step (if relevant and constant) | |
dataset_description.simulation.workflow (alpha) | STR_0D | Description of the workflow which has been used to produce this data entry (e.g. copy of the Kepler MOML if using Kepler) | ||
dataset_description.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
distribution_sources (alpha) | Sources of particles for input to kinetic equations, e.g. Fokker-Planck calculation. The sources could originate from e.g. NBI or fusion reactions. | |||
distribution_sources.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
distribution_sources.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
distribution_sources.code.name (alpha) | STR_0D | Name of software generating IDS | ||
distribution_sources.code.output_flag (alpha) | [distribution_sources.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
distribution_sources.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
distribution_sources.code.repository (alpha) | STR_0D | URL of software repository | ||
distribution_sources.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
distribution_sources.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
distribution_sources.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
distribution_sources.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
distribution_sources.ids_properties.occurrence | INT_0D | |||
distribution_sources.magnetic_axis (alpha) | STRUCTURE | Magnetic axis position (used to define a poloidal angle for the 2D profiles) | ||
distribution_sources.magnetic_axis.r (alpha) | [distribution_sources.time] | FLT_1D (uncertain) | m | Major radius |
distribution_sources.magnetic_axis.z (alpha) | [distribution_sources.time] | FLT_1D (uncertain) | m | Height |
distribution_sources.source (alpha) | [1...N] | STRUCT_ARRAY | Set of source/sink terms. A source/sink term corresponds to the particle source due to an NBI injection unit, a nuclear reaction or any combination of them (described in "identifier") | |
distribution_sources.source[:].ggd (alpha) | [distribution_sources.source[:].ggd[:].time] | STRUCT_ARRAY | Source terms in phase space (real space, velocity space, spin state), represented using the ggd, for various time slices | |
distribution_sources.source[:].ggd[:].discrete (alpha) | [1...N] | INT_1D | List of indices of grid spaces (refers to ../grid/space) for which the source is discretely distributed. For example consider a source of 3.5 MeV alpha particles provided on a grid with two coordinates (spaces); rho_tor and energy. To specify that the source is given at energies exactly equal to 3.5 MeV, let discret have length 1 and set discrete(1)=2 since energy is dimension number 2. The source is then proportional to delta( 1 - energy / 3.5MeV ), where delta is the direct delta distribution. Discrete dimensions can only be used when the grid is rectangular. | |
distribution_sources.source[:].ggd[:].grid (alpha) | STRUCTURE | Grid description | ||
distribution_sources.source[:].ggd[:].grid.grid_subset (alpha) | [1...N] | STRUCT_ARRAY | Grid subsets | |
distribution_sources.source[:].ggd[:].grid.grid_subset[:].base (alpha) | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
distribution_sources.source[:].ggd[:].grid.grid_subset[:].base[:].jacobian (alpha) | [distribution_sources.source[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
distribution_sources.source[:].ggd[:].grid.grid_subset[:].base[:].tensor_contravariant (alpha) | [distribution_sources.source[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
distribution_sources.source[:].ggd[:].grid.grid_subset[:].base[:].tensor_covariant (alpha) | [distribution_sources.source[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
distribution_sources.source[:].ggd[:].grid.grid_subset[:].dimension (alpha) | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
distribution_sources.source[:].ggd[:].grid.grid_subset[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
distribution_sources.source[:].ggd[:].grid.grid_subset[:].element[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
distribution_sources.source[:].ggd[:].grid.grid_subset[:].element[:].object[:].dimension (alpha) | INT_0D | Dimension of the object | ||
distribution_sources.source[:].ggd[:].grid.grid_subset[:].element[:].object[:].index (alpha) | INT_0D | Object index | ||
distribution_sources.source[:].ggd[:].grid.grid_subset[:].element[:].object[:].space (alpha) | INT_0D | Index of the space from which that object is taken | ||
distribution_sources.source[:].ggd[:].grid.grid_subset[:].identifier (alpha) | STRUCTURE | Grid subset identifier | ||
distribution_sources.source[:].ggd[:].grid.grid_subset[:].identifier.description (alpha) | STR_0D | Verbose description | ||
distribution_sources.source[:].ggd[:].grid.grid_subset[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distribution_sources.source[:].ggd[:].grid.grid_subset[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
distribution_sources.source[:].ggd[:].grid.grid_subset[:].metric (alpha) | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
distribution_sources.source[:].ggd[:].grid.grid_subset[:].metric.jacobian (alpha) | [distribution_sources.source[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
distribution_sources.source[:].ggd[:].grid.grid_subset[:].metric.tensor_contravariant (alpha) | [distribution_sources.source[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
distribution_sources.source[:].ggd[:].grid.grid_subset[:].metric.tensor_covariant (alpha) | [distribution_sources.source[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
distribution_sources.source[:].ggd[:].grid.identifier (alpha) | STRUCTURE | Grid identifier | ||
distribution_sources.source[:].ggd[:].grid.identifier.description (alpha) | STR_0D | Verbose description | ||
distribution_sources.source[:].ggd[:].grid.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distribution_sources.source[:].ggd[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
distribution_sources.source[:].ggd[:].grid.space (alpha) | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
distribution_sources.source[:].ggd[:].grid.space[:].coordinates_type (alpha) | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therfore defines the dimension of the space. The meaning of these predefined integer constants can be found in the documentation of the grid service library | |
distribution_sources.source[:].ggd[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier) | ||
distribution_sources.source[:].ggd[:].grid.space[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
distribution_sources.source[:].ggd[:].grid.space[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distribution_sources.source[:].ggd[:].grid.space[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
distribution_sources.source[:].ggd[:].grid.space[:].objects_per_dimension (alpha) | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
distribution_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
distribution_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary (alpha) | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
distribution_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].index (alpha) | INT_0D | Index of this (n-1)-dimensional boundary object | ||
distribution_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].neighbours (alpha) | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
distribution_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].geometry (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. |
distribution_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].measure (alpha) | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
distribution_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].nodes (alpha) | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
distribution_sources.source[:].ggd[:].particles (alpha) | [1...N] | STRUCT_ARRAY | (m.s^-1)^-3.m^-3.s^-1 | Source density of particles in phase space, for various grid subsets |
distribution_sources.source[:].ggd[:].particles[:].coefficients (alpha) | [distribution_sources.source[:].ggd[:].particles[:].values, | FLT_2D (uncertain) | (m.s^-1)^-3.m^-3.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
distribution_sources.source[:].ggd[:].particles[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
distribution_sources.source[:].ggd[:].particles[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
distribution_sources.source[:].ggd[:].particles[:].values (alpha) | [1...N] | FLT_1D (uncertain) | (m.s^-1)^-3.m^-3.s^-1 | One scalar value is provided per element in the grid subset. |
distribution_sources.source[:].ggd[:].time (alpha) | FLT_0D | s | Time | |
distribution_sources.source[:].global_quantities (alpha) | [distribution_sources.source[:].global_quantities[:].time] | STRUCT_ARRAY | Global quantities for various time slices | |
distribution_sources.source[:].global_quantities[:].particles (alpha) | FLT_0D (uncertain) | s^-1 | Particle source rate | |
distribution_sources.source[:].global_quantities[:].power (alpha) | FLT_0D (uncertain) | W | Total power of the source | |
distribution_sources.source[:].global_quantities[:].shinethrough (alpha) | STRUCTURE | Shinethrough losses | ||
distribution_sources.source[:].global_quantities[:].shinethrough.particles (alpha) | FLT_0D (uncertain) | s^-1 | Particle losses due to shinethrough | |
distribution_sources.source[:].global_quantities[:].shinethrough.power (alpha) | FLT_0D (uncertain) | W | Power losses due to shinethrough | |
distribution_sources.source[:].global_quantities[:].shinethrough.torque_tor (alpha) | FLT_0D (uncertain) | N.m | Toroidal torque losses due to shinethrough | |
distribution_sources.source[:].global_quantities[:].time (alpha) | FLT_0D | s | Time | |
distribution_sources.source[:].global_quantities[:].torque_tor (alpha) | FLT_0D (uncertain) | N.m | Total toroidal torque of the source | |
distribution_sources.source[:].gyro_type (alpha) | INT_0D | Defines how to interpret the spatial coordinates: 1 = given at the actual particle birth point; 2 =given at the gyro centre of the birth point | ||
distribution_sources.source[:].markers (alpha) | [distribution_sources.source[:].markers[:].time] | STRUCT_ARRAY | Source given as a group of markers (test particles) born per second, for various time slices | |
distribution_sources.source[:].markers[:].coordinate_identifier (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Set of coordinate identifiers, coordinates on which the markers are represented |
distribution_sources.source[:].markers[:].coordinate_identifier[:].description (alpha) | STR_0D | Verbose description | ||
distribution_sources.source[:].markers[:].coordinate_identifier[:].index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distribution_sources.source[:].markers[:].coordinate_identifier[:].name (alpha) | STR_0D | Short string identifier | ||
distribution_sources.source[:].markers[:].positions (alpha) | [distribution_sources.source[:].markers[:].weights, | FLT_2D (uncertain) | mixed | Position of the markers in the set of coordinates. The first dimension corresponds to the number of markers, the second dimension to the set of coordinates |
distribution_sources.source[:].markers[:].time (alpha) | FLT_0D | s | Time | |
distribution_sources.source[:].markers[:].weights (alpha) | [1...N] | FLT_1D (uncertain) | - | Weight of the markers, i.e. number of real particles represented by each marker. The dimension of the vector correspond to the number of markers |
distribution_sources.source[:].process (alpha) | [1...N] | STRUCT_ARRAY | Set of processes (NBI units, fusion reactions, ...) that provide the source. | |
distribution_sources.source[:].process[:].nbi_beamlets_group (alpha) | INT_0D | Index of the NBI beamlets group considered. Refers to the "unit/beamlets_group" array of the NBI IDS. 0 means sum over all beamlets groups. | ||
distribution_sources.source[:].process[:].nbi_energy (alpha) | STRUCTURE | For NBI source, energy of the accelerated species considered. index = 0 for a sum over all energies; index = 1 for full energiy; index = 2 for half energy; index = 3 for third energy | ||
distribution_sources.source[:].process[:].nbi_energy.description (alpha) | STR_0D | Verbose description | ||
distribution_sources.source[:].process[:].nbi_energy.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distribution_sources.source[:].process[:].nbi_energy.name (alpha) | STR_0D | Short string identifier | ||
distribution_sources.source[:].process[:].nbi_unit (alpha) | INT_0D | Index of the NBI unit considered. Refers to the "unit" array of the NBI IDS. 0 means sum over all NBI units. | ||
distribution_sources.source[:].process[:].reactant_energy (alpha) | STRUCTURE | For nuclear reaction source, energy of the reactants. index = 0 for a sum over all energies; index = 1 for thermal-thermal; index = 2 for beam-beam; index = 3 for beam-thermal | ||
distribution_sources.source[:].process[:].reactant_energy.description (alpha) | STR_0D | Verbose description | ||
distribution_sources.source[:].process[:].reactant_energy.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distribution_sources.source[:].process[:].reactant_energy.name (alpha) | STR_0D | Short string identifier | ||
distribution_sources.source[:].process[:].type (alpha) | STRUCTURE | Process type. index=1 for NBI; index=2 for nuclear reaction (reaction unspecified); index=3 for nuclear reaction: T(d,n)4He [D+T->He4+n]; index=4 for nuclear reaction: He3(d,p)4He [He3+D->He4+p]; index=5 for nuclear reaction: D(d,p)T [D+D->T+p]; index=6 for nuclear reaction: D(d,n)3He [D+D->He3+n]; index=7 for runaway processes | ||
distribution_sources.source[:].process[:].type.description (alpha) | STR_0D | Verbose description | ||
distribution_sources.source[:].process[:].type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distribution_sources.source[:].process[:].type.name (alpha) | STR_0D | Short string identifier | ||
distribution_sources.source[:].profiles_1d (alpha) | [distribution_sources.source[:].profiles_1d[:].time] | STRUCT_ARRAY | Source radial profiles (flux surface averaged quantities) for various time slices | |
distribution_sources.source[:].profiles_1d[:].energy (alpha) | [distribution_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source term for the energy transport equation |
distribution_sources.source[:].profiles_1d[:].grid (alpha) | STRUCTURE | Radial grid | ||
distribution_sources.source[:].profiles_1d[:].grid.area (alpha) | [distribution_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
distribution_sources.source[:].profiles_1d[:].grid.psi (alpha) | [distribution_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
distribution_sources.source[:].profiles_1d[:].grid.rho_tor (alpha) | [distribution_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
distribution_sources.source[:].profiles_1d[:].grid.rho_tor_norm (alpha) | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
distribution_sources.source[:].profiles_1d[:].grid.volume (alpha) | [distribution_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
distribution_sources.source[:].profiles_1d[:].momentum_tor (alpha) | [distribution_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Source term for the toroidal momentum equation |
distribution_sources.source[:].profiles_1d[:].particles (alpha) | [distribution_sources.source[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source term for the density transport equation |
distribution_sources.source[:].profiles_1d[:].time (alpha) | FLT_0D | s | Time | |
distribution_sources.source[:].species (alpha) | STRUCTURE | Species injected or consumed by this source/sink | ||
distribution_sources.source[:].species.ion (alpha) | STRUCTURE | Description of the ion or neutral species, used if type/index = 2 or 3 | ||
distribution_sources.source[:].species.ion.element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distribution_sources.source[:].species.ion.element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distribution_sources.source[:].species.ion.element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distribution_sources.source[:].species.ion.element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distribution_sources.source[:].species.ion.label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
distribution_sources.source[:].species.ion.state (alpha) | STRUCTURE | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | ||
distribution_sources.source[:].species.ion.state.electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distribution_sources.source[:].species.ion.state.label (alpha) | STR_0D | String identifying ion state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distribution_sources.source[:].species.ion.state.vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distribution_sources.source[:].species.ion.state.vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distribution_sources.source[:].species.ion.state.z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distribution_sources.source[:].species.ion.state.z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distribution_sources.source[:].species.ion.z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
distribution_sources.source[:].species.neutral (alpha) | STRUCTURE | Description of the neutral species, used if type/index = 4 or 5 | ||
distribution_sources.source[:].species.neutral.element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distribution_sources.source[:].species.neutral.element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distribution_sources.source[:].species.neutral.element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distribution_sources.source[:].species.neutral.element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distribution_sources.source[:].species.neutral.label (alpha) | STR_0D | String identifying neutral (e.g. H, D, T, He, C, ...) | ||
distribution_sources.source[:].species.neutral.state (alpha) | STRUCTURE | State of the species (energy, excitation, ...) | ||
distribution_sources.source[:].species.neutral.state.electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distribution_sources.source[:].species.neutral.state.label (alpha) | STR_0D | String identifying neutral state | ||
distribution_sources.source[:].species.neutral.state.neutral_type (alpha) | STRUCTURE | Neutral type, in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
distribution_sources.source[:].species.neutral.state.neutral_type.description (alpha) | STR_0D | Verbose description | ||
distribution_sources.source[:].species.neutral.state.neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distribution_sources.source[:].species.neutral.state.neutral_type.name (alpha) | STR_0D | Short string identifier | ||
distribution_sources.source[:].species.neutral.state.vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distribution_sources.source[:].species.neutral.state.vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distribution_sources.source[:].species.type (alpha) | STRUCTURE | Species type. index=1 for electron; index=2 for ion species in a single/average state (refer to ion structure); index=3 for ion species in a particular state (refer to ion/state structure); index=4 for neutral species in a single/average state (refer to neutral structure); index=5 for neutral species in a particular state (refer to neutral/state structure); index=6 for neutron; index=7 for photon | ||
distribution_sources.source[:].species.type.description (alpha) | STR_0D | Verbose description | ||
distribution_sources.source[:].species.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distribution_sources.source[:].species.type.name (alpha) | STR_0D | Short string identifier | ||
distribution_sources.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
distribution_sources.vacuum_toroidal_field (alpha) | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition) | ||
distribution_sources.vacuum_toroidal_field.b0 (alpha) | [distribution_sources.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
distribution_sources.vacuum_toroidal_field.r0 (alpha) | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
distributions (alpha) | Distribution function(s) of one or many particle species. This structure is specifically designed to handle non-Maxwellian distribution function generated during heating and current drive, typically solved using a Fokker-Planck calculation perturbed by a heating scheme (e.g. IC, EC, LH, NBI, or alpha heating) and then relaxed by Coloumb collisions. | |||
distributions.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
distributions.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
distributions.code.name (alpha) | STR_0D | Name of software generating IDS | ||
distributions.code.output_flag (alpha) | [distributions.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
distributions.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
distributions.code.repository (alpha) | STR_0D | URL of software repository | ||
distributions.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
distributions.distribution (alpha) | [1...N] | STRUCT_ARRAY | Set of distribution functions. Every distribution function has to be associated with only one particle species, specified in distri_vec/species/, but there could be multiple distribution function for each species. In this case, the fast particle populations should be superposed | |
distributions.distribution[:].fast_filter (alpha) | STRUCTURE | Description of how the fast and the thermal particle populations are separated | ||
distributions.distribution[:].fast_filter.energy (alpha) | [distributions.distribution[:].fast_filter.energy.TBD] | FLT_1D (uncertain) | eV | Energy at which the fast and thermal particle populations were separated, as a function of radius |
distributions.distribution[:].fast_filter.method (alpha) | STRUCTURE | Method used to separate the fast and thermal particle population (indices TBD) | ||
distributions.distribution[:].fast_filter.method.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].fast_filter.method.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].fast_filter.method.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].ggd (alpha) | [distributions.distribution[:].ggd[:].time] | STRUCT_ARRAY | Distribution represented using the ggd, for various time slices | |
distributions.distribution[:].ggd[:].expansion (alpha) | [1...N] | STRUCT_ARRAY | (m.s^-1)^-3.m^-3.s^-1 | Distribution function expanded into a vector of successive approximations. The first element in the vector (expansion(1)) is the zeroth order distribution function, while the K:th element in the vector (expansion(K)) is the K:th correction, such that the total distribution function is a sum over all elements in the expansion vector. |
distributions.distribution[:].ggd[:].expansion[:].grid_subset (alpha) | [1...N] | STRUCT_ARRAY | mixed | Values of the distribution function expansion, for various grid subsets |
distributions.distribution[:].ggd[:].expansion[:].grid_subset[:].coefficients (alpha) | [distributions.distribution[:].ggd[:].expansion[:].grid_subset[:].values, | FLT_2D (uncertain) | mixed | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
distributions.distribution[:].ggd[:].expansion[:].grid_subset[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
distributions.distribution[:].ggd[:].expansion[:].grid_subset[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
distributions.distribution[:].ggd[:].expansion[:].grid_subset[:].values (alpha) | [1...N] | FLT_1D (uncertain) | mixed | One scalar value is provided per element in the grid subset. |
distributions.distribution[:].ggd[:].grid (alpha) | STRUCTURE | Grid description | ||
distributions.distribution[:].ggd[:].grid.grid_subset (alpha) | [1...N] | STRUCT_ARRAY | Grid subsets | |
distributions.distribution[:].ggd[:].grid.grid_subset[:].base (alpha) | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
distributions.distribution[:].ggd[:].grid.grid_subset[:].base[:].jacobian (alpha) | [distributions.distribution[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
distributions.distribution[:].ggd[:].grid.grid_subset[:].base[:].tensor_contravariant (alpha) | [distributions.distribution[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
distributions.distribution[:].ggd[:].grid.grid_subset[:].base[:].tensor_covariant (alpha) | [distributions.distribution[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
distributions.distribution[:].ggd[:].grid.grid_subset[:].dimension (alpha) | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
distributions.distribution[:].ggd[:].grid.grid_subset[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
distributions.distribution[:].ggd[:].grid.grid_subset[:].element[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
distributions.distribution[:].ggd[:].grid.grid_subset[:].element[:].object[:].dimension (alpha) | INT_0D | Dimension of the object | ||
distributions.distribution[:].ggd[:].grid.grid_subset[:].element[:].object[:].index (alpha) | INT_0D | Object index | ||
distributions.distribution[:].ggd[:].grid.grid_subset[:].element[:].object[:].space (alpha) | INT_0D | Index of the space from which that object is taken | ||
distributions.distribution[:].ggd[:].grid.grid_subset[:].identifier (alpha) | STRUCTURE | Grid subset identifier | ||
distributions.distribution[:].ggd[:].grid.grid_subset[:].identifier.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].ggd[:].grid.grid_subset[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].ggd[:].grid.grid_subset[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].ggd[:].grid.grid_subset[:].metric (alpha) | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
distributions.distribution[:].ggd[:].grid.grid_subset[:].metric.jacobian (alpha) | [distributions.distribution[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
distributions.distribution[:].ggd[:].grid.grid_subset[:].metric.tensor_contravariant (alpha) | [distributions.distribution[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
distributions.distribution[:].ggd[:].grid.grid_subset[:].metric.tensor_covariant (alpha) | [distributions.distribution[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
distributions.distribution[:].ggd[:].grid.identifier (alpha) | STRUCTURE | Grid identifier | ||
distributions.distribution[:].ggd[:].grid.identifier.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].ggd[:].grid.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].ggd[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].ggd[:].grid.space (alpha) | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
distributions.distribution[:].ggd[:].grid.space[:].coordinates_type (alpha) | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therfore defines the dimension of the space. The meaning of these predefined integer constants can be found in the documentation of the grid service library | |
distributions.distribution[:].ggd[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier) | ||
distributions.distribution[:].ggd[:].grid.space[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].ggd[:].grid.space[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].ggd[:].grid.space[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].ggd[:].grid.space[:].objects_per_dimension (alpha) | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
distributions.distribution[:].ggd[:].grid.space[:].objects_per_dimension[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
distributions.distribution[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary (alpha) | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
distributions.distribution[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].index (alpha) | INT_0D | Index of this (n-1)-dimensional boundary object | ||
distributions.distribution[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].neighbours (alpha) | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
distributions.distribution[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].geometry (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. |
distributions.distribution[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].measure (alpha) | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
distributions.distribution[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].nodes (alpha) | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
distributions.distribution[:].ggd[:].temperature (alpha) | [distributions.distribution[:].profiles_1d.grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Reference temperature profile used to define the local thermal energy and the thermal velocity (for normalisation of the grid coordinates) |
distributions.distribution[:].ggd[:].time (alpha) | FLT_0D | s | Time | |
distributions.distribution[:].global_quantities (alpha) | [distributions.distribution[:].global_quantities[:].time] | STRUCT_ARRAY | Global quantities (integrated over plasma volume for moments of the distribution, collisional exchange and source terms), for various time slices | |
distributions.distribution[:].global_quantities[:].collisions (alpha) | STRUCTURE | Power and torque exchanged between the species described by the distribution and the different plasma species through collisions | ||
distributions.distribution[:].global_quantities[:].collisions.electrons (alpha) | STRUCTURE | Collisional exchange with electrons | ||
distributions.distribution[:].global_quantities[:].collisions.electrons.power_fast (alpha) | FLT_0D (uncertain) | W | Collisional power to the fast particle population | |
distributions.distribution[:].global_quantities[:].collisions.electrons.power_thermal (alpha) | FLT_0D (uncertain) | W | Collisional power to the thermal particle population | |
distributions.distribution[:].global_quantities[:].collisions.electrons.torque_fast_tor (alpha) | FLT_0D (uncertain) | N.m | Collisional toroidal torque to the fast particle population | |
distributions.distribution[:].global_quantities[:].collisions.electrons.torque_thermal_tor (alpha) | FLT_0D (uncertain) | N.m | Collisional toroidal torque to the thermal particle population | |
distributions.distribution[:].global_quantities[:].collisions.ion (alpha) | [1...N] | STRUCT_ARRAY | Collisional exchange with the various ion species | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
distributions.distribution[:].global_quantities[:].collisions.ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
distributions.distribution[:].global_quantities[:].collisions.ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
distributions.distribution[:].global_quantities[:].collisions.ion[:].power_fast (alpha) | FLT_0D (uncertain) | W | Collisional power to the fast particle population | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].power_thermal (alpha) | FLT_0D (uncertain) | W | Collisional power to the thermal particle population | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].power_fast (alpha) | FLT_0D (uncertain) | W | Collisional power to the fast particle population | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].power_thermal (alpha) | FLT_0D (uncertain) | W | Collisional power to the thermal particle population | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].torque_fast_tor (alpha) | FLT_0D (uncertain) | N.m | Collisional toroidal torque to the fast particle population | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].torque_thermal_tor (alpha) | FLT_0D (uncertain) | N.m | Collisional toroidal torque to the thermal particle population | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].torque_fast_tor (alpha) | FLT_0D (uncertain) | N.m | Collisional toroidal torque to the fast particle population | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].torque_thermal_tor (alpha) | FLT_0D (uncertain) | N.m | Collisional toroidal torque to the thermal particle population | |
distributions.distribution[:].global_quantities[:].collisions.ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
distributions.distribution[:].global_quantities[:].current_tor (alpha) | FLT_0D (uncertain) | N.m | Toroidal current driven by the distribution | |
distributions.distribution[:].global_quantities[:].energy (alpha) | FLT_0D (uncertain) | J | Total energy in the distribution | |
distributions.distribution[:].global_quantities[:].energy_fast (alpha) | FLT_0D (uncertain) | J | Total energy of the fast particles in the distribution | |
distributions.distribution[:].global_quantities[:].energy_fast_parallel (alpha) | FLT_0D (uncertain) | J | Parallel energy of the fast particles in the distribution | |
distributions.distribution[:].global_quantities[:].particles_fast_n (alpha) | FLT_0D (uncertain) | - | Number of fast particles in the distribution, i.e. the volume integral of the density (note: this is the number of real particles and not markers) | |
distributions.distribution[:].global_quantities[:].particles_n (alpha) | FLT_0D (uncertain) | - | Number of particles in the distribution, i.e. the volume integral of the density (note: this is the number of real particles and not markers) | |
distributions.distribution[:].global_quantities[:].source (alpha) | [1...N] | STRUCT_ARRAY | Set of volume integrated sources and sinks of particles, momentum and energy included in the Fokker-Planck modelling, related to the various waves or particle source processes affecting the distribution | |
distributions.distribution[:].global_quantities[:].source[:].identifier (alpha) | STRUCTURE | Identifier of the wave or particle source process, defined respectively in distribution/wave or distribution/process | ||
distributions.distribution[:].global_quantities[:].source[:].identifier.process_index (alpha) | INT_0D | Index into distribution/process | ||
distributions.distribution[:].global_quantities[:].source[:].identifier.type (alpha) | STRUCTURE | Type of the source term. Index = 1 for a wave, index = 2 for a particle source process | ||
distributions.distribution[:].global_quantities[:].source[:].identifier.type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].global_quantities[:].source[:].identifier.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].global_quantities[:].source[:].identifier.type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].global_quantities[:].source[:].identifier.wave_index (alpha) | INT_0D | Index into distribution/wave | ||
distributions.distribution[:].global_quantities[:].source[:].particles (alpha) | FLT_0D (uncertain) | s^-1 | Particle source rate | |
distributions.distribution[:].global_quantities[:].source[:].power (alpha) | FLT_0D (uncertain) | W | Total power of the source | |
distributions.distribution[:].global_quantities[:].source[:].torque_tor (alpha) | FLT_0D (uncertain) | N.m | Total toroidal torque of the source | |
distributions.distribution[:].global_quantities[:].time (alpha) | FLT_0D | s | Time | |
distributions.distribution[:].global_quantities[:].torque_tor_j_radial (alpha) | FLT_0D (uncertain) | N.m | Toroidal torque due to radial currents | |
distributions.distribution[:].gyro_type (alpha) | INT_0D | Defines how to interpret the spatial coordinates: 1 = given at the actual particle birth point; 2 =given at the gyro centre of the birth point | ||
distributions.distribution[:].is_delta_f (alpha) | INT_0D | If is_delta_f=1, then the distribution represents the deviation from a Maxwellian; is_delta_f=0, then the distribution represents all particles, i.e. the full-f solution | ||
distributions.distribution[:].markers (alpha) | [distributions.distribution[:].markers[:].time] | STRUCT_ARRAY | Distribution represented by a set of markers (test particles) | |
distributions.distribution[:].markers[:].coordinate_identifier (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Set of coordinate identifiers, coordinates on which the markers are represented |
distributions.distribution[:].markers[:].coordinate_identifier[:].description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].markers[:].coordinate_identifier[:].index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].markers[:].coordinate_identifier[:].name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].markers[:].positions (alpha) | [distributions.distribution[:].markers[:].weights, | FLT_2D (uncertain) | mixed | Position of the markers in the set of coordinates. The first dimension corresponds to the number of markers, the second dimension to the set of coordinates |
distributions.distribution[:].markers[:].time (alpha) | FLT_0D | s | Time | |
distributions.distribution[:].markers[:].weights (alpha) | [1...N] | FLT_1D (uncertain) | - | Weight of the markers, i.e. number of real particles represented by each marker. The dimension of the vector correspond to the number of markers |
distributions.distribution[:].process (alpha) | [1...N] | STRUCT_ARRAY | List all processes (NBI units, fusion reactions, ...) affecting the distribution, identified as in distribution_sources/source(i)/process in the DISTRIBUTION_SOURCES IDS | |
distributions.distribution[:].process[:].nbi_beamlets_group (alpha) | INT_0D | Index of the NBI beamlets group considered. Refers to the "unit/beamlets_group" array of the NBI IDS. 0 means sum over all beamlets groups. | ||
distributions.distribution[:].process[:].nbi_energy (alpha) | STRUCTURE | For NBI source, energy of the accelerated species considered. index = 0 for a sum over all energies; index = 1 for full energiy; index = 2 for half energy; index = 3 for third energy | ||
distributions.distribution[:].process[:].nbi_energy.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].process[:].nbi_energy.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].process[:].nbi_energy.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].process[:].nbi_unit (alpha) | INT_0D | Index of the NBI unit considered. Refers to the "unit" array of the NBI IDS. 0 means sum over all NBI units. | ||
distributions.distribution[:].process[:].reactant_energy (alpha) | STRUCTURE | For nuclear reaction source, energy of the reactants. index = 0 for a sum over all energies; index = 1 for thermal-thermal; index = 2 for beam-beam; index = 3 for beam-thermal | ||
distributions.distribution[:].process[:].reactant_energy.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].process[:].reactant_energy.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].process[:].reactant_energy.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].process[:].type (alpha) | STRUCTURE | Process type. index=1 for NBI; index=2 for nuclear reaction (reaction unspecified); index=3 for nuclear reaction: T(d,n)4He [D+T->He4+n]; index=4 for nuclear reaction: He3(d,p)4He [He3+D->He4+p]; index=5 for nuclear reaction: D(d,p)T [D+D->T+p]; index=6 for nuclear reaction: D(d,n)3He [D+D->He3+n]; index=7 for runaway processes | ||
distributions.distribution[:].process[:].type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].process[:].type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].process[:].type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].profiles_1d (alpha) | [distributions.distribution[:].profiles_1d[:].time] | STRUCT_ARRAY | Radial profiles (flux surface averaged quantities) for various time slices | |
distributions.distribution[:].profiles_1d[:].co_passing (alpha) | STRUCTURE | Flux surface averaged profile evaluated using the co-passing particle part of the distribution. | ||
distributions.distribution[:].profiles_1d[:].co_passing.collisions (alpha) | STRUCTURE | Power and torque exchanged between the species described by the distribution and the different plasma species through collisions | ||
distributions.distribution[:].profiles_1d[:].co_passing.collisions.electrons (alpha) | STRUCTURE | Collisional exchange with electrons | ||
distributions.distribution[:].profiles_1d[:].co_passing.collisions.electrons.power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.electrons.power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.electrons.torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.electrons.torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion (alpha) | [1...N] | STRUCT_ARRAY | Collisional exchange with the various ion species | |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].co_passing.collisions.ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
distributions.distribution[:].profiles_1d[:].co_passing.current_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Total toroidal driven current density of fast (non-thermal) particles (excluding electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_1d[:].co_passing.current_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Total toroidal driven current density (including electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_1d[:].co_passing.density (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
distributions.distribution[:].profiles_1d[:].co_passing.density_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast particles |
distributions.distribution[:].profiles_1d[:].co_passing.pressure (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure (thermal+non-thermal) |
distributions.distribution[:].profiles_1d[:].co_passing.pressure_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure of fast particles |
distributions.distribution[:].profiles_1d[:].co_passing.pressure_fast_parallel (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure of fast particles in the parallel direction |
distributions.distribution[:].profiles_1d[:].co_passing.source (alpha) | [1...N] | STRUCT_ARRAY | Set of flux averaged sources and sinks of particles, momentum and energy included in the Fokker-Planck modelling, related to the various waves or particle source processes affecting the distribution | |
distributions.distribution[:].profiles_1d[:].co_passing.source[:].energy (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source rate of energy density |
distributions.distribution[:].profiles_1d[:].co_passing.source[:].identifier (alpha) | STRUCTURE | Identifier of the wave or particle source process, defined respectively in distribution/wave or distribution/process | ||
distributions.distribution[:].profiles_1d[:].co_passing.source[:].identifier.process_index (alpha) | INT_0D | Index into distribution/process | ||
distributions.distribution[:].profiles_1d[:].co_passing.source[:].identifier.type (alpha) | STRUCTURE | Type of the source term. Index = 1 for a wave, index = 2 for a particle source process | ||
distributions.distribution[:].profiles_1d[:].co_passing.source[:].identifier.type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].profiles_1d[:].co_passing.source[:].identifier.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].profiles_1d[:].co_passing.source[:].identifier.type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].profiles_1d[:].co_passing.source[:].identifier.wave_index (alpha) | INT_0D | Index into distribution/wave | ||
distributions.distribution[:].profiles_1d[:].co_passing.source[:].momentum_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Source rate of toroidal angular momentum density |
distributions.distribution[:].profiles_1d[:].co_passing.source[:].particles (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source rate of thermal particle density |
distributions.distribution[:].profiles_1d[:].co_passing.torque_tor_j_radial (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Toroidal torque due to radial currents |
distributions.distribution[:].profiles_1d[:].collisions (alpha) | STRUCTURE | Power and torque exchanged between the species described by the distribution and the different plasma species through collisions | ||
distributions.distribution[:].profiles_1d[:].collisions.electrons (alpha) | STRUCTURE | Collisional exchange with electrons | ||
distributions.distribution[:].profiles_1d[:].collisions.electrons.power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].collisions.electrons.power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].collisions.electrons.torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].collisions.electrons.torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].collisions.ion (alpha) | [1...N] | STRUCT_ARRAY | Collisional exchange with the various ion species | |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
distributions.distribution[:].profiles_1d[:].collisions.ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
distributions.distribution[:].profiles_1d[:].collisions.ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
distributions.distribution[:].profiles_1d[:].collisions.ion[:].power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].collisions.ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
distributions.distribution[:].profiles_1d[:].counter_passing (alpha) | STRUCTURE | Flux surface averaged profile evaluated using the counter-passing particle part of the distribution. | ||
distributions.distribution[:].profiles_1d[:].counter_passing.collisions (alpha) | STRUCTURE | Power and torque exchanged between the species described by the distribution and the different plasma species through collisions | ||
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.electrons (alpha) | STRUCTURE | Collisional exchange with electrons | ||
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.electrons.power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.electrons.power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.electrons.torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.electrons.torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion (alpha) | [1...N] | STRUCT_ARRAY | Collisional exchange with the various ion species | |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].counter_passing.collisions.ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
distributions.distribution[:].profiles_1d[:].counter_passing.current_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Total toroidal driven current density of fast (non-thermal) particles (excluding electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_1d[:].counter_passing.current_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Total toroidal driven current density (including electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_1d[:].counter_passing.density (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
distributions.distribution[:].profiles_1d[:].counter_passing.density_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast particles |
distributions.distribution[:].profiles_1d[:].counter_passing.pressure (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure (thermal+non-thermal) |
distributions.distribution[:].profiles_1d[:].counter_passing.pressure_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure of fast particles |
distributions.distribution[:].profiles_1d[:].counter_passing.pressure_fast_parallel (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure of fast particles in the parallel direction |
distributions.distribution[:].profiles_1d[:].counter_passing.source (alpha) | [1...N] | STRUCT_ARRAY | Set of flux averaged sources and sinks of particles, momentum and energy included in the Fokker-Planck modelling, related to the various waves or particle source processes affecting the distribution | |
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].energy (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source rate of energy density |
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].identifier (alpha) | STRUCTURE | Identifier of the wave or particle source process, defined respectively in distribution/wave or distribution/process | ||
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].identifier.process_index (alpha) | INT_0D | Index into distribution/process | ||
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].identifier.type (alpha) | STRUCTURE | Type of the source term. Index = 1 for a wave, index = 2 for a particle source process | ||
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].identifier.type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].identifier.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].identifier.type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].identifier.wave_index (alpha) | INT_0D | Index into distribution/wave | ||
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].momentum_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Source rate of toroidal angular momentum density |
distributions.distribution[:].profiles_1d[:].counter_passing.source[:].particles (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source rate of thermal particle density |
distributions.distribution[:].profiles_1d[:].counter_passing.torque_tor_j_radial (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Toroidal torque due to radial currents |
distributions.distribution[:].profiles_1d[:].current_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Total toroidal driven current density of fast (non-thermal) particles (excluding electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_1d[:].current_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Total toroidal driven current density (including electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_1d[:].density (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
distributions.distribution[:].profiles_1d[:].density_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast particles |
distributions.distribution[:].profiles_1d[:].grid (alpha) | STRUCTURE | Radial grid | ||
distributions.distribution[:].profiles_1d[:].grid.area (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
distributions.distribution[:].profiles_1d[:].grid.psi (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
distributions.distribution[:].profiles_1d[:].grid.rho_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm (alpha) | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
distributions.distribution[:].profiles_1d[:].grid.volume (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
distributions.distribution[:].profiles_1d[:].pressure (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure (thermal+non-thermal) |
distributions.distribution[:].profiles_1d[:].pressure_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure of fast particles |
distributions.distribution[:].profiles_1d[:].pressure_fast_parallel (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure of fast particles in the parallel direction |
distributions.distribution[:].profiles_1d[:].source (alpha) | [1...N] | STRUCT_ARRAY | Set of flux averaged sources and sinks of particles, momentum and energy included in the Fokker-Planck modelling, related to the various waves or particle source processes affecting the distribution | |
distributions.distribution[:].profiles_1d[:].source[:].energy (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source rate of energy density |
distributions.distribution[:].profiles_1d[:].source[:].identifier (alpha) | STRUCTURE | Identifier of the wave or particle source process, defined respectively in distribution/wave or distribution/process | ||
distributions.distribution[:].profiles_1d[:].source[:].identifier.process_index (alpha) | INT_0D | Index into distribution/process | ||
distributions.distribution[:].profiles_1d[:].source[:].identifier.type (alpha) | STRUCTURE | Type of the source term. Index = 1 for a wave, index = 2 for a particle source process | ||
distributions.distribution[:].profiles_1d[:].source[:].identifier.type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].profiles_1d[:].source[:].identifier.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].profiles_1d[:].source[:].identifier.type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].profiles_1d[:].source[:].identifier.wave_index (alpha) | INT_0D | Index into distribution/wave | ||
distributions.distribution[:].profiles_1d[:].source[:].momentum_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Source rate of toroidal angular momentum density |
distributions.distribution[:].profiles_1d[:].source[:].particles (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source rate of thermal particle density |
distributions.distribution[:].profiles_1d[:].thermalisation (alpha) | STRUCTURE | Flux surface averaged source of thermal particles, momentum and energy due to thermalisation. Here thermalisation refers to non-thermal particles, sufficiently assimilated to the thermal background to be re-categorised as thermal particles. Note that this source may also be negative if thermal particles are being accelerated such that they form a distinct non-thermal contribution, e.g. due run-away of RF interactions. | ||
distributions.distribution[:].profiles_1d[:].thermalisation.energy (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source rate of energy density within the thermal particle population due to the thermalisation of fast particles |
distributions.distribution[:].profiles_1d[:].thermalisation.momentum_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Source rate of toroidal angular momentum density within the thermal particle population due to the thermalisation of fast particles |
distributions.distribution[:].profiles_1d[:].thermalisation.particles (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source rate of thermal particle density due to the thermalisation of fast particles |
distributions.distribution[:].profiles_1d[:].time (alpha) | FLT_0D | s | Time | |
distributions.distribution[:].profiles_1d[:].torque_tor_j_radial (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Toroidal torque due to radial currents |
distributions.distribution[:].profiles_1d[:].trapped (alpha) | STRUCTURE | Flux surface averaged profile evaluated using the trapped particle part of the distribution. | ||
distributions.distribution[:].profiles_1d[:].trapped.collisions (alpha) | STRUCTURE | Power and torque exchanged between the species described by the distribution and the different plasma species through collisions | ||
distributions.distribution[:].profiles_1d[:].trapped.collisions.electrons (alpha) | STRUCTURE | Collisional exchange with electrons | ||
distributions.distribution[:].profiles_1d[:].trapped.collisions.electrons.power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.electrons.power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.electrons.torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.electrons.torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion (alpha) | [1...N] | STRUCT_ARRAY | Collisional exchange with the various ion species | |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].power_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].power_thermal (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].torque_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_1d[:].trapped.collisions.ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
distributions.distribution[:].profiles_1d[:].trapped.current_fast_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Total toroidal driven current density of fast (non-thermal) particles (excluding electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_1d[:].trapped.current_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Total toroidal driven current density (including electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_1d[:].trapped.density (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
distributions.distribution[:].profiles_1d[:].trapped.density_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast particles |
distributions.distribution[:].profiles_1d[:].trapped.pressure (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure (thermal+non-thermal) |
distributions.distribution[:].profiles_1d[:].trapped.pressure_fast (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure of fast particles |
distributions.distribution[:].profiles_1d[:].trapped.pressure_fast_parallel (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | J.m^-3 | Pressure of fast particles in the parallel direction |
distributions.distribution[:].profiles_1d[:].trapped.source (alpha) | [1...N] | STRUCT_ARRAY | Set of flux averaged sources and sinks of particles, momentum and energy included in the Fokker-Planck modelling, related to the various waves or particle source processes affecting the distribution | |
distributions.distribution[:].profiles_1d[:].trapped.source[:].energy (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Source rate of energy density |
distributions.distribution[:].profiles_1d[:].trapped.source[:].identifier (alpha) | STRUCTURE | Identifier of the wave or particle source process, defined respectively in distribution/wave or distribution/process | ||
distributions.distribution[:].profiles_1d[:].trapped.source[:].identifier.process_index (alpha) | INT_0D | Index into distribution/process | ||
distributions.distribution[:].profiles_1d[:].trapped.source[:].identifier.type (alpha) | STRUCTURE | Type of the source term. Index = 1 for a wave, index = 2 for a particle source process | ||
distributions.distribution[:].profiles_1d[:].trapped.source[:].identifier.type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].profiles_1d[:].trapped.source[:].identifier.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].profiles_1d[:].trapped.source[:].identifier.type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].profiles_1d[:].trapped.source[:].identifier.wave_index (alpha) | INT_0D | Index into distribution/wave | ||
distributions.distribution[:].profiles_1d[:].trapped.source[:].momentum_tor (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Source rate of toroidal angular momentum density |
distributions.distribution[:].profiles_1d[:].trapped.source[:].particles (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | s^-1.m^-3 | Source rate of thermal particle density |
distributions.distribution[:].profiles_1d[:].trapped.torque_tor_j_radial (alpha) | [distributions.distribution[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | N.m^-2 | Toroidal torque due to radial currents |
distributions.distribution[:].profiles_2d (alpha) | [distributions.distribution[:].profiles_2d[:].time] | STRUCT_ARRAY | 2D profiles in the poloidal plane for various time slices | |
distributions.distribution[:].profiles_2d[:].co_passing (alpha) | STRUCTURE | Flux surface averaged profile evaluated using the co-passing particle part of the distribution. | ||
distributions.distribution[:].profiles_2d[:].co_passing.collisions (alpha) | STRUCTURE | Power and torque exchanged between the species described by the distribution and the different plasma species through collisions | ||
distributions.distribution[:].profiles_2d[:].co_passing.collisions.electrons (alpha) | STRUCTURE | Collisional exchange with electrons | ||
distributions.distribution[:].profiles_2d[:].co_passing.collisions.electrons.power_fast (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.electrons.power_thermal (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.electrons.torque_fast_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.electrons.torque_thermal_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion (alpha) | [1...N] | STRUCT_ARRAY | Collisional exchange with the various ion species | |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].power_fast (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].power_thermal (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].power_fast (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].power_thermal (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].torque_fast_tor (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].torque_thermal_tor (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].torque_fast_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].torque_thermal_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].co_passing.collisions.ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
distributions.distribution[:].profiles_2d[:].co_passing.current_fast_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | A.m^-2 | Total toroidal driven current density of fast (non-thermal) particles (excluding electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_2d[:].co_passing.current_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | A.m^-2 | Total toroidal driven current density (including electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_2d[:].co_passing.density (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | m^-3 | Density (thermal+non-thermal) |
distributions.distribution[:].profiles_2d[:].co_passing.density_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | m^-3 | Density of fast particles |
distributions.distribution[:].profiles_2d[:].co_passing.pressure (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | J.m^-3 | Pressure (thermal+non-thermal) |
distributions.distribution[:].profiles_2d[:].co_passing.pressure_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | J.m^-3 | Pressure of fast particles |
distributions.distribution[:].profiles_2d[:].co_passing.pressure_fast_parallel (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | J.m^-3 | Pressure of fast particles in the parallel direction |
distributions.distribution[:].profiles_2d[:].co_passing.torque_tor_j_radial (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Toroidal torque due to radial currents |
distributions.distribution[:].profiles_2d[:].collisions (alpha) | STRUCTURE | Power and torque exchanged between the species described by the distribution and the different plasma species through collisions | ||
distributions.distribution[:].profiles_2d[:].collisions.electrons (alpha) | STRUCTURE | Collisional exchange with electrons | ||
distributions.distribution[:].profiles_2d[:].collisions.electrons.power_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].collisions.electrons.power_thermal (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].collisions.electrons.torque_fast_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].collisions.electrons.torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].collisions.ion (alpha) | [1...N] | STRUCT_ARRAY | Collisional exchange with the various ion species | |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
distributions.distribution[:].profiles_2d[:].collisions.ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
distributions.distribution[:].profiles_2d[:].collisions.ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
distributions.distribution[:].profiles_2d[:].collisions.ion[:].power_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].power_thermal (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].power_fast (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].power_thermal (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].torque_fast_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].torque_thermal_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].torque_fast_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].torque_thermal_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].collisions.ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
distributions.distribution[:].profiles_2d[:].counter_passing (alpha) | STRUCTURE | Flux surface averaged profile evaluated using the counter-passing particle part of the distribution. | ||
distributions.distribution[:].profiles_2d[:].counter_passing.collisions (alpha) | STRUCTURE | Power and torque exchanged between the species described by the distribution and the different plasma species through collisions | ||
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.electrons (alpha) | STRUCTURE | Collisional exchange with electrons | ||
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.electrons.power_fast (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.electrons.power_thermal (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.electrons.torque_fast_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.electrons.torque_thermal_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion (alpha) | [1...N] | STRUCT_ARRAY | Collisional exchange with the various ion species | |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].power_fast (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].power_thermal (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].power_fast (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].power_thermal (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].torque_fast_tor (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].torque_thermal_tor (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].torque_fast_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].torque_thermal_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].counter_passing.collisions.ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
distributions.distribution[:].profiles_2d[:].counter_passing.current_fast_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | A.m^-2 | Total toroidal driven current density of fast (non-thermal) particles (excluding electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_2d[:].counter_passing.current_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | A.m^-2 | Total toroidal driven current density (including electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_2d[:].counter_passing.density (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | m^-3 | Density (thermal+non-thermal) |
distributions.distribution[:].profiles_2d[:].counter_passing.density_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | m^-3 | Density of fast particles |
distributions.distribution[:].profiles_2d[:].counter_passing.pressure (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | J.m^-3 | Pressure (thermal+non-thermal) |
distributions.distribution[:].profiles_2d[:].counter_passing.pressure_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | J.m^-3 | Pressure of fast particles |
distributions.distribution[:].profiles_2d[:].counter_passing.pressure_fast_parallel (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | J.m^-3 | Pressure of fast particles in the parallel direction |
distributions.distribution[:].profiles_2d[:].counter_passing.torque_tor_j_radial (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Toroidal torque due to radial currents |
distributions.distribution[:].profiles_2d[:].current_fast_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.r, | FLT_2D (uncertain) | A.m^-2 | Total toroidal driven current density of fast (non-thermal) particles (excluding electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_2d[:].current_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.r, | FLT_2D (uncertain) | A.m^-2 | Total toroidal driven current density (including electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_2d[:].density (alpha) | [distributions.distribution[:].profiles_2d[:].grid.r, | FLT_2D (uncertain) | m^-3 | Density (thermal+non-thermal) |
distributions.distribution[:].profiles_2d[:].density_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.r, | FLT_2D (uncertain) | m^-3 | Density of fast particles |
distributions.distribution[:].profiles_2d[:].grid (alpha) | STRUCTURE | Grid. The grid has to be rectangular in a pair of coordinates, as specified in type | ||
distributions.distribution[:].profiles_2d[:].grid.area (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
distributions.distribution[:].profiles_2d[:].grid.psi (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
distributions.distribution[:].profiles_2d[:].grid.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
distributions.distribution[:].profiles_2d[:].grid.rho_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm (alpha) | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation) |
distributions.distribution[:].profiles_2d[:].grid.theta_geometric (alpha) | [1...N] | FLT_1D (uncertain) | rad | Geometrical poloidal angle |
distributions.distribution[:].profiles_2d[:].grid.theta_straight (alpha) | [1...N] | FLT_1D (uncertain) | rad | Straight field line poloidal angle |
distributions.distribution[:].profiles_2d[:].grid.type (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm] | STRUCTURE | m^3 | Grid type: index=0: Rectangular grid in the (R,Z) coordinates; index=1: Rectangular grid in the (radial, theta_geometric) coordinates; index=2: Rectangular grid in the (radial, theta_straight) coordinates. |
distributions.distribution[:].profiles_2d[:].grid.type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].profiles_2d[:].grid.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].profiles_2d[:].grid.type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].profiles_2d[:].grid.volume (alpha) | [distributions.distribution[:].profiles_2d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
distributions.distribution[:].profiles_2d[:].grid.z (alpha) | [1...N] | FLT_1D (uncertain) | m | Height |
distributions.distribution[:].profiles_2d[:].pressure (alpha) | [distributions.distribution[:].profiles_2d[:].grid.r, | FLT_2D (uncertain) | J.m^-3 | Pressure (thermal+non-thermal) |
distributions.distribution[:].profiles_2d[:].pressure_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.r, | FLT_2D (uncertain) | J.m^-3 | Pressure of fast particles |
distributions.distribution[:].profiles_2d[:].pressure_fast_parallel (alpha) | [distributions.distribution[:].profiles_2d[:].grid.r, | FLT_2D (uncertain) | J.m^-3 | Pressure of fast particles in the parallel direction |
distributions.distribution[:].profiles_2d[:].time (alpha) | FLT_0D | s | Time | |
distributions.distribution[:].profiles_2d[:].torque_tor_j_radial (alpha) | [distributions.distribution[:].profiles_2d[:].grid.r, | FLT_2D (uncertain) | N.m^-2 | Toroidal torque due to radial currents |
distributions.distribution[:].profiles_2d[:].trapped (alpha) | STRUCTURE | Flux surface averaged profile evaluated using the trapped particle part of the distribution. | ||
distributions.distribution[:].profiles_2d[:].trapped.collisions (alpha) | STRUCTURE | Power and torque exchanged between the species described by the distribution and the different plasma species through collisions | ||
distributions.distribution[:].profiles_2d[:].trapped.collisions.electrons (alpha) | STRUCTURE | Collisional exchange with electrons | ||
distributions.distribution[:].profiles_2d[:].trapped.collisions.electrons.power_fast (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.electrons.power_thermal (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.electrons.torque_fast_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.electrons.torque_thermal_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion (alpha) | [1...N] | STRUCT_ARRAY | Collisional exchange with the various ion species | |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].power_fast (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].power_thermal (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].power_fast (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the fast particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].power_thermal (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Collisional power density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].torque_fast_tor (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].torque_thermal_tor (alpha) | [distributions.grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].torque_fast_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the fast particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].torque_thermal_tor (alpha) | [distributions.distribution[:].grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Collisional toroidal torque density to the thermal particle population |
distributions.distribution[:].profiles_2d[:].trapped.collisions.ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
distributions.distribution[:].profiles_2d[:].trapped.current_fast_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | A.m^-2 | Total toroidal driven current density of fast (non-thermal) particles (excluding electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_2d[:].trapped.current_tor (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | A.m^-2 | Total toroidal driven current density (including electron and thermal ion back-current, or drag-current) |
distributions.distribution[:].profiles_2d[:].trapped.density (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | m^-3 | Density (thermal+non-thermal) |
distributions.distribution[:].profiles_2d[:].trapped.density_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | m^-3 | Density of fast particles |
distributions.distribution[:].profiles_2d[:].trapped.pressure (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | J.m^-3 | Pressure (thermal+non-thermal) |
distributions.distribution[:].profiles_2d[:].trapped.pressure_fast (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | J.m^-3 | Pressure of fast particles |
distributions.distribution[:].profiles_2d[:].trapped.pressure_fast_parallel (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | J.m^-3 | Pressure of fast particles in the parallel direction |
distributions.distribution[:].profiles_2d[:].trapped.torque_tor_j_radial (alpha) | [distributions.distribution[:].profiles_2d[:].grid.grid.rho_tor_norm, | FLT_2D (uncertain) | N.m^-2 | Toroidal torque due to radial currents |
distributions.distribution[:].species (alpha) | STRUCTURE | Species described by this distribution | ||
distributions.distribution[:].species.ion (alpha) | STRUCTURE | Description of the ion or neutral species, used if type/index = 2 or 3 | ||
distributions.distribution[:].species.ion.element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].species.ion.element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].species.ion.element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].species.ion.element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].species.ion.label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
distributions.distribution[:].species.ion.state (alpha) | STRUCTURE | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | ||
distributions.distribution[:].species.ion.state.electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].species.ion.state.label (alpha) | STR_0D | String identifying ion state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
distributions.distribution[:].species.ion.state.vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].species.ion.state.vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].species.ion.state.z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
distributions.distribution[:].species.ion.state.z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
distributions.distribution[:].species.ion.z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
distributions.distribution[:].species.neutral (alpha) | STRUCTURE | Description of the neutral species, used if type/index = 4 or 5 | ||
distributions.distribution[:].species.neutral.element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
distributions.distribution[:].species.neutral.element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
distributions.distribution[:].species.neutral.element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
distributions.distribution[:].species.neutral.element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
distributions.distribution[:].species.neutral.label (alpha) | STR_0D | String identifying neutral (e.g. H, D, T, He, C, ...) | ||
distributions.distribution[:].species.neutral.state (alpha) | STRUCTURE | State of the species (energy, excitation, ...) | ||
distributions.distribution[:].species.neutral.state.electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
distributions.distribution[:].species.neutral.state.label (alpha) | STR_0D | String identifying neutral state | ||
distributions.distribution[:].species.neutral.state.neutral_type (alpha) | STRUCTURE | Neutral type, in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
distributions.distribution[:].species.neutral.state.neutral_type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].species.neutral.state.neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].species.neutral.state.neutral_type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].species.neutral.state.vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
distributions.distribution[:].species.neutral.state.vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
distributions.distribution[:].species.type (alpha) | STRUCTURE | Species type. index=1 for electron; index=2 for ion species in a single/average state (refer to ion structure); index=3 for ion species in a particular state (refer to ion/state structure); index=4 for neutral species in a single/average state (refer to neutral structure); index=5 for neutral species in a particular state (refer to neutral/state structure); index=6 for neutron; index=7 for photon | ||
distributions.distribution[:].species.type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].species.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].species.type.name (alpha) | STR_0D | Short string identifier | ||
distributions.distribution[:].wave (alpha) | [1...N] | STRUCT_ARRAY | List all waves affecting the distribution, identified as in waves/coherent_wave(i)/identifier in the waves IDS | |
distributions.distribution[:].wave[:].antenna_name (alpha) | STR_0D | Name of the antenna that launches this wave. Corresponds to the name specified in antennas/ec(i)/name, or antennas/ic(i)/name or antennas/lh(i)/name (depends of antenna/wave type) in the ANTENNAS IDS. | ||
distributions.distribution[:].wave[:].index_in_antenna (alpha) | INT_0D | Index of the wave (starts at 1), separating different waves generated from a single antenna. | ||
distributions.distribution[:].wave[:].type (alpha) | STRUCTURE | Wave/antenna type. index=1 for name=EC; index=2 for name=IC; index=3 for name=LH | ||
distributions.distribution[:].wave[:].type.description (alpha) | STR_0D | Verbose description | ||
distributions.distribution[:].wave[:].type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
distributions.distribution[:].wave[:].type.name (alpha) | STR_0D | Short string identifier | ||
distributions.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
distributions.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
distributions.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
distributions.ids_properties.occurrence | INT_0D | |||
distributions.magnetic_axis (alpha) | STRUCTURE | Magnetic axis position (used to define a poloidal angle for the 2D profiles) | ||
distributions.magnetic_axis.r (alpha) | [distributions.time] | FLT_1D (uncertain) | m | Major radius |
distributions.magnetic_axis.z (alpha) | [distributions.time] | FLT_1D (uncertain) | m | Height |
distributions.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
distributions.vacuum_toroidal_field (alpha) | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities) | ||
distributions.vacuum_toroidal_field.b0 (alpha) | [distributions.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
distributions.vacuum_toroidal_field.r0 (alpha) | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
ec_antennas (alpha) | Antenna systems for heating and current drive in the electron cyclotron (EC) frequencies. | |||
ec_antennas.antenna (alpha) | [1...N] | STRUCT_ARRAY | Set of Electron Cyclotron antennas | |
ec_antennas.antenna[:].beam (alpha) | STRUCTURE | Beam characteristics | ||
ec_antennas.antenna[:].beam.phase (alpha) | STRUCTURE | Phase ellipse characteristics | ||
ec_antennas.antenna[:].beam.phase.angle (alpha) | STRUCTURE | Rotation angle for the phase ellipse | ||
ec_antennas.antenna[:].beam.phase.angle.data (alpha) | [ec_antennas.antenna[:].beam.phase.angle.time] | FLT_1D (uncertain) | rad | Rotation angle for the phase ellipse |
ec_antennas.antenna[:].beam.phase.angle.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].beam.phase.curvature (alpha) | STRUCTURE | Inverse curvature radii for the phase ellipse, positive/negative for divergent/convergent beams | ||
ec_antennas.antenna[:].beam.phase.curvature.data (alpha) | [1...2, | FLT_2D (uncertain) | m^-1 | Inverse curvature radii for the phase ellipse, positive/negative for divergent/convergent beams |
ec_antennas.antenna[:].beam.phase.curvature.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].beam.spot (alpha) | STRUCTURE | Spot ellipse characteristics | ||
ec_antennas.antenna[:].beam.spot.angle (alpha) | STRUCTURE | Rotation angle for the spot ellipse | ||
ec_antennas.antenna[:].beam.spot.angle.data (alpha) | [ec_antennas.antenna[:].beam.spot.angle.time] | FLT_1D (uncertain) | rad | Rotation angle for the spot ellipse |
ec_antennas.antenna[:].beam.spot.angle.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].beam.spot.size (alpha) | STRUCTURE | Size of the spot ellipse | ||
ec_antennas.antenna[:].beam.spot.size.data (alpha) | [1...2, | FLT_2D (uncertain) | m | Size of the spot ellipse |
ec_antennas.antenna[:].beam.spot.size.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].frequency (alpha) | FLT_0D (uncertain) | Hz | Frequency | |
ec_antennas.antenna[:].launching_angle_pol (alpha) | STRUCTURE | Poloidal launching angle between the horizontal plane and the poloidal component of the nominal beam centerline. tan(angle_pol)=-k_z/k_R; | ||
ec_antennas.antenna[:].launching_angle_pol.data (alpha) | [ec_antennas.antenna[:].launching_angle_pol.time] | FLT_1D (uncertain) | rad | Poloidal launching angle between the horizontal plane and the poloidal component of the nominal beam centerline. tan(angle_pol)=-k_z/k_R; |
ec_antennas.antenna[:].launching_angle_pol.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].launching_angle_tor (alpha) | STRUCTURE | Toroidal launching angle between the poloidal plane and the nominal beam centerline. sin(angle_tor)=k_phi | ||
ec_antennas.antenna[:].launching_angle_tor.data (alpha) | [ec_antennas.antenna[:].launching_angle_tor.time] | FLT_1D (uncertain) | rad | Toroidal launching angle between the poloidal plane and the nominal beam centerline. sin(angle_tor)=k_phi |
ec_antennas.antenna[:].launching_angle_tor.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].launching_position (alpha) | STRUCTURE | Launching position of the beam | ||
ec_antennas.antenna[:].launching_position.phi (alpha) | STRUCTURE | Toroidal angle | ||
ec_antennas.antenna[:].launching_position.phi.data (alpha) | [ec_antennas.antenna[:].launching_position.phi.time] | FLT_1D (uncertain) | rad | Toroidal angle |
ec_antennas.antenna[:].launching_position.phi.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].launching_position.r (alpha) | STRUCTURE | Major radius | ||
ec_antennas.antenna[:].launching_position.r.data (alpha) | [ec_antennas.antenna[:].launching_position.r.time] | FLT_1D (uncertain) | m | Major radius |
ec_antennas.antenna[:].launching_position.r.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].launching_position.z (alpha) | STRUCTURE | Height | ||
ec_antennas.antenna[:].launching_position.z.data (alpha) | [ec_antennas.antenna[:].launching_position.z.time] | FLT_1D (uncertain) | m | Height |
ec_antennas.antenna[:].launching_position.z.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].mode (alpha) | STRUCTURE | Incoming wave mode (+ or -1 for O/X mode) | ||
ec_antennas.antenna[:].mode.data (alpha) | [ec_antennas.antenna[:].mode.time] | INT_1D | Incoming wave mode (+ or -1 for O/X mode) | |
ec_antennas.antenna[:].mode.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.antenna[:].name (alpha) | STR_0D | Name of the antenna | ||
ec_antennas.antenna[:].power (alpha) | STRUCTURE | Power | ||
ec_antennas.antenna[:].power.data (alpha) | [ec_antennas.antenna[:].power.time] | FLT_1D (uncertain) | W | Power |
ec_antennas.antenna[:].power.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ec_antennas.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
ec_antennas.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
ec_antennas.code.name (alpha) | STR_0D | Name of software generating IDS | ||
ec_antennas.code.output_flag (alpha) | [ec_antennas.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
ec_antennas.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
ec_antennas.code.repository (alpha) | STR_0D | URL of software repository | ||
ec_antennas.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
ec_antennas.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
ec_antennas.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
ec_antennas.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
ec_antennas.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
ece (alpha) | Electron cyclotron emission diagnostic | |||
ece.channel (alpha) | [1...N] | STRUCT_ARRAY | Set of channels (frequency) | |
ece.channel[:].frequency (alpha) | FLT_0D (uncertain) | Hz | Frequency of the channel | |
ece.channel[:].harmonic (alpha) | STRUCTURE | Harmonic detected by the channel | ||
ece.channel[:].harmonic.data (alpha) | [ece.channel[:].harmonic.time] | INT_1D | Harmonic detected by the channel | |
ece.channel[:].harmonic.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ece.channel[:].identifier (alpha) | STR_0D | ID of the channel | ||
ece.channel[:].name (alpha) | STR_0D | Name of the channel | ||
ece.channel[:].position (alpha) | STRUCTURE | Position of the measurements | ||
ece.channel[:].position.phi (alpha) | STRUCTURE | Toroidal angle | ||
ece.channel[:].position.phi.data (alpha) | [ece.channel[:].position.phi.time] | FLT_1D (uncertain) | rad | Toroidal angle |
ece.channel[:].position.phi.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ece.channel[:].position.r (alpha) | STRUCTURE | Major radius | ||
ece.channel[:].position.r.data (alpha) | [ece.channel[:].position.r.time] | FLT_1D (uncertain) | m | Major radius |
ece.channel[:].position.r.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ece.channel[:].position.z (alpha) | STRUCTURE | Height | ||
ece.channel[:].position.z.data (alpha) | [ece.channel[:].position.z.time] | FLT_1D (uncertain) | m | Height |
ece.channel[:].position.z.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ece.channel[:].t_e (alpha) | STRUCTURE | Electron temperature | ||
ece.channel[:].t_e.data (alpha) | [ece.channel[:].t_e.time] | FLT_1D (uncertain) | eV | Electron temperature |
ece.channel[:].t_e.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ece.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
ece.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
ece.code.name (alpha) | STR_0D | Name of software generating IDS | ||
ece.code.output_flag (alpha) | [ece.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
ece.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
ece.code.repository (alpha) | STR_0D | URL of software repository | ||
ece.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
ece.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
ece.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
ece.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
ece.ids_properties.occurrence | INT_0D | |||
ece.line_of_sight (alpha) | STRUCTURE | Description of the line of sight of the diagnostic (valid for all channels), defined by two points | ||
ece.line_of_sight.first_point (alpha) | STRUCTURE | Position of the first point | ||
ece.line_of_sight.first_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
ece.line_of_sight.first_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
ece.line_of_sight.first_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
ece.line_of_sight.second_point (alpha) | STRUCTURE | Position of the second point | ||
ece.line_of_sight.second_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
ece.line_of_sight.second_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
ece.line_of_sight.second_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
ece.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
edge_profiles (alpha) | Edge plasma profiles (includes the scrape-off layer and possibly part of the confined plasma) | |||
edge_profiles.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
edge_profiles.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_profiles.code.name (alpha) | STR_0D | Name of software generating IDS | ||
edge_profiles.code.output_flag (alpha) | [edge_profiles.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
edge_profiles.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
edge_profiles.code.repository (alpha) | STR_0D | URL of software repository | ||
edge_profiles.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_profiles.ggd (alpha) | [edge_profiles.ggd[:].time] | STRUCT_ARRAY | Edge plasma quantities represented using the general grid description, for various time slices | |
edge_profiles.ggd[:].e_field (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Electric field, given on various grid subsets |
edge_profiles.ggd[:].e_field[:].diamagnetic (alpha) | [edge_profiles.ggd[:].e_field[:].radial] | FLT_1D (uncertain) | V.m^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].e_field[:].radial, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].e_field[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].e_field[:].parallel (alpha) | [edge_profiles.ggd[:].e_field[:].radial] | FLT_1D (uncertain) | V.m^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].e_field[:].radial, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].poloidal (alpha) | [edge_profiles.ggd[:].e_field[:].radial] | FLT_1D (uncertain) | V.m^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].e_field[:].radial, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].e_field[:].radial, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].e_field[:].toroidal (alpha) | [edge_profiles.ggd[:].e_field[:].radial] | FLT_1D (uncertain) | V.m^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].e_field[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].e_field[:].radial, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
edge_profiles.ggd[:].electrons.density (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].electrons.density[:].coefficients (alpha) | [edge_profiles.ggd[:].electrons.density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.density[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.density[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].electrons.density[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.density_fast (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles, given on various grid subsets |
edge_profiles.ggd[:].electrons.density_fast[:].coefficients (alpha) | [edge_profiles.ggd[:].electrons.density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.density_fast[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.density_fast[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].electrons.density_fast[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.distribution_function (alpha) | [1...N] | STRUCT_ARRAY | mixed | Distribution function, given on various grid subsets |
edge_profiles.ggd[:].electrons.distribution_function[:].coefficients (alpha) | [edge_profiles.ggd[:].electrons.distribution_function[:].values, | FLT_2D (uncertain) | mixed | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.distribution_function[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.distribution_function[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].electrons.distribution_function[:].values (alpha) | [1...N] | FLT_1D (uncertain) | mixed | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.pressure (alpha) | [1...N] | STRUCT_ARRAY | Pa | Pressure, given on various grid subsets |
edge_profiles.ggd[:].electrons.pressure[:].coefficients (alpha) | [edge_profiles.ggd[:].electrons.pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.pressure[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.pressure[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].electrons.pressure[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.pressure_fast_parallel (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure, given on various grid subsets |
edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].coefficients (alpha) | [edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].electrons.pressure_fast_parallel[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure, given on various grid subsets |
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].coefficients (alpha) | [edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].electrons.pressure_fast_perpendicular[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.temperature (alpha) | [1...N] | STRUCT_ARRAY | eV | Temperature, given on various grid subsets |
edge_profiles.ggd[:].electrons.temperature[:].coefficients (alpha) | [edge_profiles.ggd[:].electrons.temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.temperature[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.temperature[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].electrons.temperature[:].values (alpha) | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity (alpha) | [1...N] | STRUCTURE | m.s^-1 | Velocity, given on various grid subsets |
edge_profiles.ggd[:].electrons.velocity.diamagnetic (alpha) | [edge_profiles.ggd[:].electrons.velocity.radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity.diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].electrons.velocity.radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity.grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].electrons.velocity.grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].electrons.velocity.parallel (alpha) | [edge_profiles.ggd[:].electrons.velocity.radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity.parallel_coefficients (alpha) | [edge_profiles.ggd[:].electrons.velocity.radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity.poloidal (alpha) | [edge_profiles.ggd[:].electrons.velocity.radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity.poloidal_coefficients (alpha) | [edge_profiles.ggd[:].electrons.velocity.radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity.radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity.radial_coefficients (alpha) | [edge_profiles.ggd[:].electrons.velocity.radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].electrons.velocity.toroidal (alpha) | [edge_profiles.ggd[:].electrons.velocity.radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].electrons.velocity.toroidal_coefficients (alpha) | [edge_profiles.ggd[:].electrons.velocity.radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].grid (alpha) | STRUCTURE | Grid description | ||
edge_profiles.ggd[:].grid.grid_subset (alpha) | [1...N] | STRUCT_ARRAY | Grid subsets | |
edge_profiles.ggd[:].grid.grid_subset[:].base (alpha) | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
edge_profiles.ggd[:].grid.grid_subset[:].base[:].jacobian (alpha) | [edge_profiles.ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_profiles.ggd[:].grid.grid_subset[:].base[:].tensor_contravariant (alpha) | [edge_profiles.ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_profiles.ggd[:].grid.grid_subset[:].base[:].tensor_covariant (alpha) | [edge_profiles.ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_profiles.ggd[:].grid.grid_subset[:].dimension (alpha) | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
edge_profiles.ggd[:].grid.grid_subset[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
edge_profiles.ggd[:].grid.grid_subset[:].element[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
edge_profiles.ggd[:].grid.grid_subset[:].element[:].object[:].dimension (alpha) | INT_0D | Dimension of the object | ||
edge_profiles.ggd[:].grid.grid_subset[:].element[:].object[:].index (alpha) | INT_0D | Object index | ||
edge_profiles.ggd[:].grid.grid_subset[:].element[:].object[:].space (alpha) | INT_0D | Index of the space from which that object is taken | ||
edge_profiles.ggd[:].grid.grid_subset[:].identifier (alpha) | STRUCTURE | Grid subset identifier | ||
edge_profiles.ggd[:].grid.grid_subset[:].identifier.description (alpha) | STR_0D | Verbose description | ||
edge_profiles.ggd[:].grid.grid_subset[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_profiles.ggd[:].grid.grid_subset[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
edge_profiles.ggd[:].grid.grid_subset[:].metric (alpha) | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
edge_profiles.ggd[:].grid.grid_subset[:].metric.jacobian (alpha) | [edge_profiles.ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_profiles.ggd[:].grid.grid_subset[:].metric.tensor_contravariant (alpha) | [edge_profiles.ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_profiles.ggd[:].grid.grid_subset[:].metric.tensor_covariant (alpha) | [edge_profiles.ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_profiles.ggd[:].grid.identifier (alpha) | STRUCTURE | Grid identifier | ||
edge_profiles.ggd[:].grid.identifier.description (alpha) | STR_0D | Verbose description | ||
edge_profiles.ggd[:].grid.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_profiles.ggd[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
edge_profiles.ggd[:].grid.space (alpha) | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
edge_profiles.ggd[:].grid.space[:].coordinates_type (alpha) | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therfore defines the dimension of the space. The meaning of these predefined integer constants can be found in the documentation of the grid service library | |
edge_profiles.ggd[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier) | ||
edge_profiles.ggd[:].grid.space[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
edge_profiles.ggd[:].grid.space[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_profiles.ggd[:].grid.space[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
edge_profiles.ggd[:].grid.space[:].objects_per_dimension (alpha) | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
edge_profiles.ggd[:].grid.space[:].objects_per_dimension[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
edge_profiles.ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary (alpha) | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
edge_profiles.ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].index (alpha) | INT_0D | Index of this (n-1)-dimensional boundary object | ||
edge_profiles.ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].neighbours (alpha) | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
edge_profiles.ggd[:].grid.space[:].objects_per_dimension[:].object[:].geometry (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. |
edge_profiles.ggd[:].grid.space[:].objects_per_dimension[:].object[:].measure (alpha) | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
edge_profiles.ggd[:].grid.space[:].objects_per_dimension[:].object[:].nodes (alpha) | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
edge_profiles.ggd[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
edge_profiles.ggd[:].ion[:].density (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal) (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].density[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].density[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].density[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].density[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].density_fast (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].density_fast[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].density_fast[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].density_fast[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].density_fast[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_profiles.ggd[:].ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_profiles.ggd[:].ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_profiles.ggd[:].ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_profiles.ggd[:].ion[:].energy_density_kinetic (alpha) | [1...N] | STRUCT_ARRAY | J.m^-3 | Kinetic energy density (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].values, | FLT_2D (uncertain) | J.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].energy_density_kinetic[:].values (alpha) | [1...N] | FLT_1D (uncertain) | J.m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
edge_profiles.ggd[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_profiles.ggd[:].ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
edge_profiles.ggd[:].ion[:].pressure (alpha) | [1...N] | STRUCT_ARRAY | Pa | Pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].pressure[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].pressure[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].pressure[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].pressure[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].pressure_fast_parallel (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].pressure_fast_parallel[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].pressure_fast_perpendicular[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
edge_profiles.ggd[:].ion[:].state[:].density (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].density[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].density[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].density[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].density[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].density_fast (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].density_fast[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].density_fast[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].density_fast[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].density_fast[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].distribution_function (alpha) | [1...N] | STRUCT_ARRAY | mixed | Distribution function, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].values, | FLT_2D (uncertain) | mixed | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].distribution_function[:].values (alpha) | [1...N] | FLT_1D (uncertain) | mixed | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic (alpha) | [1...N] | STRUCT_ARRAY | J.m^-3 | Kinetic energy density, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].values, | FLT_2D (uncertain) | J.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].energy_density_kinetic[:].values (alpha) | [1...N] | FLT_1D (uncertain) | J.m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential (alpha) | [1...N] | STRUCT_ARRAY | Elementary Charge Unit | Cumulative and average ionisation potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z'=0 to z-1)), where Epot is the ionisation potential of ion Xz_+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].values, | FLT_2D (uncertain) | Elementary Charge Unit | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].ionisation_potential[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Elementary Charge Unit | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
edge_profiles.ggd[:].ion[:].state[:].pressure (alpha) | [1...N] | STRUCT_ARRAY | Pa | Pressure, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].pressure[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].pressure[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].pressure[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].pressure[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_parallel[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].pressure_fast_perpendicular[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].temperature (alpha) | [1...N] | STRUCT_ARRAY | eV | Temperature, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].temperature[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].temperature[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].temperature[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].temperature[:].values (alpha) | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].diamagnetic (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].velocity[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].velocity[:].parallel (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].poloidal (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].toroidal (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity due to the diamagnetic drift, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].diamagnetic (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].parallel (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].poloidal (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].toroidal (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity due to the ExB drift, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].diamagnetic (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].parallel (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].poloidal (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].toroidal (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_profiles.ggd[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_profiles.ggd[:].ion[:].state[:].z_average (alpha) | [1...N] | STRUCT_ARRAY | Elementary Charge Unit | Average Z of the charge state bundle (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].z_average[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].z_average[:].values, | FLT_2D (uncertain) | Elementary Charge Unit | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].z_average[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].z_average[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].z_average[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Elementary Charge Unit | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
edge_profiles.ggd[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
edge_profiles.ggd[:].ion[:].state[:].z_square_average (alpha) | [1...N] | STRUCT_ARRAY | Elementary Charge Unit | Average Z square of the charge state bundle (equal to z_min if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle, given on various grid subsets |
edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].values, | FLT_2D (uncertain) | Elementary Charge Unit | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].state[:].z_square_average[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Elementary Charge Unit | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].temperature (alpha) | [1...N] | STRUCT_ARRAY | eV | Temperature (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].temperature[:].coefficients (alpha) | [edge_profiles.ggd[:].ion[:].temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].temperature[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].temperature[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].temperature[:].values (alpha) | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].ion[:].velocity[:].diamagnetic (alpha) | [edge_profiles.ggd[:].ion[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].ion[:].velocity[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].ion[:].velocity[:].parallel (alpha) | [edge_profiles.ggd[:].ion[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].poloidal (alpha) | [edge_profiles.ggd[:].ion[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].velocity[:].toroidal (alpha) | [edge_profiles.ggd[:].ion[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].ion[:].velocity[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].ion[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
edge_profiles.ggd[:].j_anomalous (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Anomalous current density, given on various grid subsets |
edge_profiles.ggd[:].j_anomalous[:].diamagnetic (alpha) | [edge_profiles.ggd[:].j_anomalous[:].radial] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].j_anomalous[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_anomalous[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].j_anomalous[:].parallel (alpha) | [edge_profiles.ggd[:].j_anomalous[:].radial] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].j_anomalous[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].poloidal (alpha) | [edge_profiles.ggd[:].j_anomalous[:].radial] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].j_anomalous[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].j_anomalous[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_anomalous[:].toroidal (alpha) | [edge_profiles.ggd[:].j_anomalous[:].radial] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_anomalous[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].j_anomalous[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to the diamgnetic drift, given on various grid subsets |
edge_profiles.ggd[:].j_diamagnetic[:].diamagnetic (alpha) | [edge_profiles.ggd[:].j_diamagnetic[:].radial] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].j_diamagnetic[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_diamagnetic[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].j_diamagnetic[:].parallel (alpha) | [edge_profiles.ggd[:].j_diamagnetic[:].radial] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].j_diamagnetic[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].poloidal (alpha) | [edge_profiles.ggd[:].j_diamagnetic[:].radial] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].j_diamagnetic[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].j_diamagnetic[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_diamagnetic[:].toroidal (alpha) | [edge_profiles.ggd[:].j_diamagnetic[:].radial] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_diamagnetic[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].j_diamagnetic[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to the heat viscosity, given on various grid subsets |
edge_profiles.ggd[:].j_heat_viscosity[:].diamagnetic (alpha) | [edge_profiles.ggd[:].j_heat_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].j_heat_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_heat_viscosity[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].j_heat_viscosity[:].parallel (alpha) | [edge_profiles.ggd[:].j_heat_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].j_heat_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].poloidal (alpha) | [edge_profiles.ggd[:].j_heat_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].j_heat_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].j_heat_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_heat_viscosity[:].toroidal (alpha) | [edge_profiles.ggd[:].j_heat_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_heat_viscosity[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].j_heat_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Inertial current density, given on various grid subsets |
edge_profiles.ggd[:].j_inertial[:].diamagnetic (alpha) | [edge_profiles.ggd[:].j_inertial[:].radial] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].j_inertial[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_inertial[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].j_inertial[:].parallel (alpha) | [edge_profiles.ggd[:].j_inertial[:].radial] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].j_inertial[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].poloidal (alpha) | [edge_profiles.ggd[:].j_inertial[:].radial] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].j_inertial[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].j_inertial[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_inertial[:].toroidal (alpha) | [edge_profiles.ggd[:].j_inertial[:].radial] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_inertial[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].j_inertial[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to ion neutral friction, given on various grid subsets |
edge_profiles.ggd[:].j_ion_neutral_friction[:].diamagnetic (alpha) | [edge_profiles.ggd[:].j_ion_neutral_friction[:].radial] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].j_ion_neutral_friction[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_ion_neutral_friction[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].j_ion_neutral_friction[:].parallel (alpha) | [edge_profiles.ggd[:].j_ion_neutral_friction[:].radial] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].j_ion_neutral_friction[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].poloidal (alpha) | [edge_profiles.ggd[:].j_ion_neutral_friction[:].radial] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].j_ion_neutral_friction[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].j_ion_neutral_friction[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_ion_neutral_friction[:].toroidal (alpha) | [edge_profiles.ggd[:].j_ion_neutral_friction[:].radial] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_ion_neutral_friction[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].j_ion_neutral_friction[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to the parallel viscosity, given on various grid subsets |
edge_profiles.ggd[:].j_parallel_viscosity[:].diamagnetic (alpha) | [edge_profiles.ggd[:].j_parallel_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].j_parallel_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_parallel_viscosity[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].j_parallel_viscosity[:].parallel (alpha) | [edge_profiles.ggd[:].j_parallel_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].j_parallel_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].poloidal (alpha) | [edge_profiles.ggd[:].j_parallel_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].j_parallel_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].j_parallel_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_parallel_viscosity[:].toroidal (alpha) | [edge_profiles.ggd[:].j_parallel_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_parallel_viscosity[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].j_parallel_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to the perpendicular viscosity, given on various grid subsets |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].diamagnetic (alpha) | [edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_perpendicular_viscosity[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].j_perpendicular_viscosity[:].parallel (alpha) | [edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].poloidal (alpha) | [edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].toroidal (alpha) | [edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_perpendicular_viscosity[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].j_perpendicular_viscosity[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density due to Pfirsch-Schlüter effects, given on various grid subsets |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].diamagnetic (alpha) | [edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial] | FLT_1D (uncertain) | A.m^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].j_pfirsch_schlueter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].j_pfirsch_schlueter[:].parallel (alpha) | [edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial] | FLT_1D (uncertain) | A.m^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].poloidal (alpha) | [edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial] | FLT_1D (uncertain) | A.m^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].toroidal (alpha) | [edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial] | FLT_1D (uncertain) | A.m^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].j_pfirsch_schlueter[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].j_pfirsch_schlueter[:].radial, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].n_i_total_over_n_e (alpha) | [1...N] | STRUCT_ARRAY | - | Ratio of total ion density (sum over ion species) over electron density. (thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].n_i_total_over_n_e[:].coefficients (alpha) | [edge_profiles.ggd[:].n_i_total_over_n_e[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].n_i_total_over_n_e[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].n_i_total_over_n_e[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].n_i_total_over_n_e[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different neutral species | |
edge_profiles.ggd[:].neutral[:].density (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal) (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].density[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].density[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].density[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].density[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].density_fast (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].density_fast[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].density_fast[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].density_fast[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].density_fast[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_profiles.ggd[:].neutral[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_profiles.ggd[:].neutral[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_profiles.ggd[:].neutral[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_profiles.ggd[:].neutral[:].energy_density_kinetic (alpha) | [1...N] | STRUCT_ARRAY | J.m^-3 | Kinetic energy density (sum over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].values, | FLT_2D (uncertain) | J.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].energy_density_kinetic[:].values (alpha) | [1...N] | FLT_1D (uncertain) | J.m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].ion_index (alpha) | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
edge_profiles.ggd[:].neutral[:].label (alpha) | STR_0D | String identifying the species (e.g. H, D, T, He, C, D2, DT, CD4, ...) | ||
edge_profiles.ggd[:].neutral[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_profiles.ggd[:].neutral[:].pressure (alpha) | [1...N] | STRUCT_ARRAY | Pa | Pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].pressure[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].pressure[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].pressure[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].pressure[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].pressure_fast_parallel[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].pressure_fast_perpendicular[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Quantities related to the different states of the species (energy, excitation, ...) | |
edge_profiles.ggd[:].neutral[:].state[:].density (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density (thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].density[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].density[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].density[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].density[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].density[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].density_fast (alpha) | [1...N] | STRUCT_ARRAY | m^-3 | Density of fast (non-thermal) particles, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].values, | FLT_2D (uncertain) | m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].density_fast[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].distribution_function (alpha) | [1...N] | STRUCT_ARRAY | mixed | Distribution function, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].values, | FLT_2D (uncertain) | mixed | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].distribution_function[:].values (alpha) | [1...N] | FLT_1D (uncertain) | mixed | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic (alpha) | [1...N] | STRUCT_ARRAY | J.m^-3 | Kinetic energy density, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].values, | FLT_2D (uncertain) | J.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].energy_density_kinetic[:].values (alpha) | [1...N] | FLT_1D (uncertain) | J.m^-3 | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].label (alpha) | STR_0D | String identifying state | ||
edge_profiles.ggd[:].neutral[:].state[:].neutral_type (alpha) | STRUCTURE | Neutral type, in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
edge_profiles.ggd[:].neutral[:].state[:].neutral_type.description (alpha) | STR_0D | Verbose description | ||
edge_profiles.ggd[:].neutral[:].state[:].neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_profiles.ggd[:].neutral[:].state[:].neutral_type.name (alpha) | STR_0D | Short string identifier | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure (alpha) | [1...N] | STRUCT_ARRAY | Pa | Pressure, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].pressure[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].pressure[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].pressure[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) parallel pressure, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_parallel[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular (alpha) | [1...N] | STRUCT_ARRAY | Pa | Fast (non-thermal) perpendicular pressure, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].pressure_fast_perpendicular[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].temperature (alpha) | [1...N] | STRUCT_ARRAY | eV | Temperature, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].temperature[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].temperature[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].temperature[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].temperature[:].values (alpha) | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].diamagnetic (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].parallel (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].poloidal (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].toroidal (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity due to the diamagnetic drift, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].diamagnetic (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].parallel (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].poloidal (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].toroidal (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_diamagnetic[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity due to the ExB drift, given on various grid subsets |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].diamagnetic (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].parallel (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].poloidal (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].toroidal (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].state[:].velocity_exb[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_profiles.ggd[:].neutral[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_profiles.ggd[:].neutral[:].temperature (alpha) | [1...N] | STRUCT_ARRAY | eV | Temperature (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].temperature[:].coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].temperature[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].temperature[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].temperature[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].temperature[:].values (alpha) | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Velocity (average over states when multiple states are considered), given on various grid subsets |
edge_profiles.ggd[:].neutral[:].velocity[:].diamagnetic (alpha) | [edge_profiles.ggd[:].neutral[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].diamagnetic_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].neutral[:].velocity[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].neutral[:].velocity[:].parallel (alpha) | [edge_profiles.ggd[:].neutral[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].parallel_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].poloidal (alpha) | [edge_profiles.ggd[:].neutral[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].poloidal_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].radial_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].neutral[:].velocity[:].toroidal (alpha) | [edge_profiles.ggd[:].neutral[:].velocity[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].neutral[:].velocity[:].toroidal_coefficients (alpha) | [edge_profiles.ggd[:].neutral[:].velocity[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].pressure_parallel (alpha) | [1...N] | STRUCT_ARRAY | Pa | Total parallel pressure (electrons+ions, thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].pressure_parallel[:].coefficients (alpha) | [edge_profiles.ggd[:].pressure_parallel[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].pressure_parallel[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].pressure_parallel[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].pressure_parallel[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].pressure_perpendicular (alpha) | [1...N] | STRUCT_ARRAY | Pa | Total perpendicular pressure (electrons+ions, thermal+non-thermal), given on various grid subsets |
edge_profiles.ggd[:].pressure_perpendicular[:].coefficients (alpha) | [edge_profiles.ggd[:].pressure_perpendicular[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].pressure_perpendicular[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].pressure_perpendicular[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].pressure_perpendicular[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].pressure_thermal (alpha) | [1...N] | STRUCT_ARRAY | Pa | Thermal pressure (electrons+ions), given on various grid subsets |
edge_profiles.ggd[:].pressure_thermal[:].coefficients (alpha) | [edge_profiles.ggd[:].pressure_thermal[:].values, | FLT_2D (uncertain) | Pa | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].pressure_thermal[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].pressure_thermal[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].pressure_thermal[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Pa | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].t_i_average (alpha) | [1...N] | STRUCT_ARRAY | eV | Ion temperature (averaged on ion species), given on various grid subsets |
edge_profiles.ggd[:].t_i_average[:].coefficients (alpha) | [edge_profiles.ggd[:].t_i_average[:].values, | FLT_2D (uncertain) | eV | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].t_i_average[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].t_i_average[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].t_i_average[:].values (alpha) | [1...N] | FLT_1D (uncertain) | eV | One scalar value is provided per element in the grid subset. |
edge_profiles.ggd[:].time (alpha) | FLT_0D | s | Time | |
edge_profiles.ggd[:].zeff (alpha) | [1...N] | STRUCT_ARRAY | - | Effective charge, given on various grid subsets |
edge_profiles.ggd[:].zeff[:].coefficients (alpha) | [edge_profiles.ggd[:].zeff[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_profiles.ggd[:].zeff[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_profiles.ggd[:].zeff[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_profiles.ggd[:].zeff[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_profiles.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
edge_profiles.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
edge_profiles.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
edge_profiles.ids_properties.occurrence | INT_0D | |||
edge_profiles.profiles_1d (alpha) | [edge_profiles.profiles_1d[:].time] | STRUCT_ARRAY | SOL radial profiles for various time slices, taken on outboard equatorial mid-plane | |
edge_profiles.profiles_1d[:].conductivity_parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | ohm^-1.m^-1 | Parallel conductivity |
edge_profiles.profiles_1d[:].e_field (alpha) | STRUCTURE | V.m^-1 | Electric field, averaged on the magnetic surface. E.g for the parellel component, average(E.B) / B0, using core_profiles/vacuum_toroidal_field/b0 | |
edge_profiles.profiles_1d[:].e_field.diamagnetic (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].e_field.parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Parallel component |
edge_profiles.profiles_1d[:].e_field.poloidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Poloidal component |
edge_profiles.profiles_1d[:].e_field.radial (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Radial component |
edge_profiles.profiles_1d[:].e_field.toroidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Toroidal component |
edge_profiles.profiles_1d[:].e_field_parallel (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Parallel electric field = average(E.B) / B0, where Core_Profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
edge_profiles.profiles_1d[:].electrons.density (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
edge_profiles.profiles_1d[:].electrons.density_fast (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
edge_profiles.profiles_1d[:].electrons.pressure (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
edge_profiles.profiles_1d[:].electrons.pressure_fast_parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
edge_profiles.profiles_1d[:].electrons.pressure_fast_perpendicular (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
edge_profiles.profiles_1d[:].electrons.temperature (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
edge_profiles.profiles_1d[:].electrons.velocity (alpha) | STRUCTURE | m.s^-1 | Velocity | |
edge_profiles.profiles_1d[:].electrons.velocity.diamagnetic (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].electrons.velocity.parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].electrons.velocity.poloidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].electrons.velocity.radial (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].electrons.velocity.toroidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].electrons.velocity_pol (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
edge_profiles.profiles_1d[:].electrons.velocity_tor (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
edge_profiles.profiles_1d[:].grid (alpha) | STRUCTURE | Radial grid | ||
edge_profiles.profiles_1d[:].grid.area (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
edge_profiles.profiles_1d[:].grid.psi (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
edge_profiles.profiles_1d[:].grid.rho_tor (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
edge_profiles.profiles_1d[:].grid.rho_tor_norm (alpha) | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
edge_profiles.profiles_1d[:].grid.volume (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
edge_profiles.profiles_1d[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
edge_profiles.profiles_1d[:].ion[:].density (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].density_fast (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_profiles.profiles_1d[:].ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_profiles.profiles_1d[:].ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_profiles.profiles_1d[:].ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_profiles.profiles_1d[:].ion[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
edge_profiles.profiles_1d[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_profiles.profiles_1d[:].ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
edge_profiles.profiles_1d[:].ion[:].pressure (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].pressure_fast_parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].pressure_fast_perpendicular (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].state (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
edge_profiles.profiles_1d[:].ion[:].state[:].density (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
edge_profiles.profiles_1d[:].ion[:].state[:].density_fast (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
edge_profiles.profiles_1d[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_profiles.profiles_1d[:].ion[:].state[:].ionisation_potential (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Cumulative and average ionisation potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z'=0 to z-1)), where Epot is the ionisation potential of ion Xz’+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
edge_profiles.profiles_1d[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
edge_profiles.profiles_1d[:].ion[:].state[:].pressure (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
edge_profiles.profiles_1d[:].ion[:].state[:].pressure_fast_parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
edge_profiles.profiles_1d[:].ion[:].state[:].pressure_fast_perpendicular (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
edge_profiles.profiles_1d[:].ion[:].state[:].temperature (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity (alpha) | STRUCTURE | m.s^-1 | Velocity | |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.diamagnetic (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.poloidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.radial (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].ion[:].state[:].velocity.toroidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_profiles.profiles_1d[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_profiles.profiles_1d[:].ion[:].state[:].z_average (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Average Z of the charge state bundle (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
edge_profiles.profiles_1d[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
edge_profiles.profiles_1d[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
edge_profiles.profiles_1d[:].ion[:].state[:].z_square_average (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Average Z square of the charge state bundle (equal to z_min if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
edge_profiles.profiles_1d[:].ion[:].temperature (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].velocity (alpha) | STRUCTURE | m.s^-1 | Velocity (average over charge states when multiple charge states are considered) | |
edge_profiles.profiles_1d[:].ion[:].velocity.diamagnetic (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].ion[:].velocity.parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].ion[:].velocity.poloidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].ion[:].velocity.radial (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].ion[:].velocity.toroidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].ion[:].velocity_pol (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity (average over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].velocity_tor (obsolescent) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity (average over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed), volume averaged over plasma radius | |
edge_profiles.profiles_1d[:].ion[:].z_ion_1d (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Average charge of the ion species (sum of states charge weighted by state density and divided by ion density) |
edge_profiles.profiles_1d[:].ion[:].z_ion_square_1d (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Average sqare charge of the ion species (sum of states square charge weighted by state density and divided by ion density) |
edge_profiles.profiles_1d[:].j_bootstrap (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Bootstrap current density = average(J_Bootstrap.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].j_non_inductive (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Non-inductive (includes bootstrap) parallel current density = average(jni.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].j_ohmic (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Ohmic parallel current density = average(J_Ohmic.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].j_tor (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Total toroidal current density = average(J_Tor/R) / average(1/R) |
edge_profiles.profiles_1d[:].j_total (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Total parallel current density = average(jtot.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
edge_profiles.profiles_1d[:].magnetic_shear (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor |
edge_profiles.profiles_1d[:].momentum_tor (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | kg.m^-1.s^-1 | Total plasma toroidal momentum, summed over ion species and electrons weighted by their density and major radius, i.e. sum_over_species(n*R*m*Vphi) |
edge_profiles.profiles_1d[:].n_i_total_over_n_e (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal) |
edge_profiles.profiles_1d[:].neutral (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different neutral species | |
edge_profiles.profiles_1d[:].neutral[:].density (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].density_fast (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_profiles.profiles_1d[:].neutral[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_profiles.profiles_1d[:].neutral[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_profiles.profiles_1d[:].neutral[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_profiles.profiles_1d[:].neutral[:].ion_index (alpha) | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
edge_profiles.profiles_1d[:].neutral[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
edge_profiles.profiles_1d[:].neutral[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_profiles.profiles_1d[:].neutral[:].pressure (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].pressure_fast_parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].pressure_fast_perpendicular (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].state (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (energy, excitation, ...) | |
edge_profiles.profiles_1d[:].neutral[:].state[:].density (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
edge_profiles.profiles_1d[:].neutral[:].state[:].density_fast (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
edge_profiles.profiles_1d[:].neutral[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].neutral_type (alpha) | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].neutral_type.description (alpha) | STR_0D | Verbose description | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].neutral_type.name (alpha) | STR_0D | Short string identifier | ||
edge_profiles.profiles_1d[:].neutral[:].state[:].pressure (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (thermal+non-thermal) |
edge_profiles.profiles_1d[:].neutral[:].state[:].pressure_fast_parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
edge_profiles.profiles_1d[:].neutral[:].state[:].pressure_fast_perpendicular (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
edge_profiles.profiles_1d[:].neutral[:].state[:].temperature (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity (alpha) | STRUCTURE | m.s^-1 | Velocity | |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.diamagnetic (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.poloidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.radial (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].neutral[:].state[:].velocity.toroidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].neutral[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_profiles.profiles_1d[:].neutral[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_profiles.profiles_1d[:].neutral[:].temperature (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
edge_profiles.profiles_1d[:].neutral[:].velocity (alpha) | STRUCTURE | m.s^-1 | Velocity (average over charge states when multiple charge states are considered) | |
edge_profiles.profiles_1d[:].neutral[:].velocity.diamagnetic (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component |
edge_profiles.profiles_1d[:].neutral[:].velocity.parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Parallel component |
edge_profiles.profiles_1d[:].neutral[:].velocity.poloidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal component |
edge_profiles.profiles_1d[:].neutral[:].velocity.radial (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Radial component |
edge_profiles.profiles_1d[:].neutral[:].velocity.toroidal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal component |
edge_profiles.profiles_1d[:].pressure_ion_total (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total (sum over ion species) thermal ion pressure |
edge_profiles.profiles_1d[:].pressure_parallel (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total parallel pressure (electrons+ions, thermal+non-thermal) |
edge_profiles.profiles_1d[:].pressure_perpendicular (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total perpendicular pressure (electrons+ions, thermal+non-thermal) |
edge_profiles.profiles_1d[:].pressure_thermal (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Thermal pressure (electrons+ions) |
edge_profiles.profiles_1d[:].q (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Safety factor |
edge_profiles.profiles_1d[:].t_i_average (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Ion temperature (averaged on charge states and ion species) |
edge_profiles.profiles_1d[:].time (alpha) | FLT_0D | s | Time | |
edge_profiles.profiles_1d[:].zeff (alpha) | [edge_profiles.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Effective charge |
edge_profiles.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
edge_sources (alpha) | Edge plasma sources. Energy terms correspond to the full kinetic energy equation (i.e. the energy flux takes into account the energy transported by the particle flux) | |||
edge_sources.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
edge_sources.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_sources.code.name (alpha) | STR_0D | Name of software generating IDS | ||
edge_sources.code.output_flag (alpha) | [edge_sources.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
edge_sources.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
edge_sources.code.repository (alpha) | STR_0D | URL of software repository | ||
edge_sources.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_sources.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
edge_sources.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
edge_sources.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
edge_sources.ids_properties.occurrence | INT_0D | |||
edge_sources.source (alpha) | [1...N] | STRUCT_ARRAY | Set of source terms | |
edge_sources.source[:].ggd (alpha) | [edge_sources.source[:].ggd[:].time] | STRUCT_ARRAY | Source terms represented using the general grid description, for various time slices | |
edge_sources.source[:].ggd[:].current (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density source |
edge_sources.source[:].ggd[:].current[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].current[:].values, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].current[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].current[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].current[:].values (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].electrons (alpha) | STRUCTURE | Sources for electrons | ||
edge_sources.source[:].ggd[:].electrons.energy (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Source term for the electron energy equation, given on various grid subsets |
edge_sources.source[:].ggd[:].electrons.energy[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].electrons.energy[:].values, | FLT_2D (uncertain) | W.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].electrons.energy[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].electrons.energy[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].electrons.energy[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].electrons.particles (alpha) | [1...N] | STRUCT_ARRAY | m^-3.s^-1 | Source term for electron density equation, given on various grid subsets |
edge_sources.source[:].ggd[:].electrons.particles[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].electrons.particles[:].values, | FLT_2D (uncertain) | m^-3.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].electrons.particles[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].electrons.particles[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].electrons.particles[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-3.s^-1 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].grid (alpha) | STRUCTURE | Grid description | ||
edge_sources.source[:].ggd[:].grid.grid_subset (alpha) | [1...N] | STRUCT_ARRAY | Grid subsets | |
edge_sources.source[:].ggd[:].grid.grid_subset[:].base (alpha) | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
edge_sources.source[:].ggd[:].grid.grid_subset[:].base[:].jacobian (alpha) | [edge_sources.source[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_sources.source[:].ggd[:].grid.grid_subset[:].base[:].tensor_contravariant (alpha) | [edge_sources.source[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_sources.source[:].ggd[:].grid.grid_subset[:].base[:].tensor_covariant (alpha) | [edge_sources.source[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_sources.source[:].ggd[:].grid.grid_subset[:].dimension (alpha) | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
edge_sources.source[:].ggd[:].grid.grid_subset[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
edge_sources.source[:].ggd[:].grid.grid_subset[:].element[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
edge_sources.source[:].ggd[:].grid.grid_subset[:].element[:].object[:].dimension (alpha) | INT_0D | Dimension of the object | ||
edge_sources.source[:].ggd[:].grid.grid_subset[:].element[:].object[:].index (alpha) | INT_0D | Object index | ||
edge_sources.source[:].ggd[:].grid.grid_subset[:].element[:].object[:].space (alpha) | INT_0D | Index of the space from which that object is taken | ||
edge_sources.source[:].ggd[:].grid.grid_subset[:].identifier (alpha) | STRUCTURE | Grid subset identifier | ||
edge_sources.source[:].ggd[:].grid.grid_subset[:].identifier.description (alpha) | STR_0D | Verbose description | ||
edge_sources.source[:].ggd[:].grid.grid_subset[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_sources.source[:].ggd[:].grid.grid_subset[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
edge_sources.source[:].ggd[:].grid.grid_subset[:].metric (alpha) | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
edge_sources.source[:].ggd[:].grid.grid_subset[:].metric.jacobian (alpha) | [edge_sources.source[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_sources.source[:].ggd[:].grid.grid_subset[:].metric.tensor_contravariant (alpha) | [edge_sources.source[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_sources.source[:].ggd[:].grid.grid_subset[:].metric.tensor_covariant (alpha) | [edge_sources.source[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_sources.source[:].ggd[:].grid.identifier (alpha) | STRUCTURE | Grid identifier | ||
edge_sources.source[:].ggd[:].grid.identifier.description (alpha) | STR_0D | Verbose description | ||
edge_sources.source[:].ggd[:].grid.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_sources.source[:].ggd[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
edge_sources.source[:].ggd[:].grid.space (alpha) | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
edge_sources.source[:].ggd[:].grid.space[:].coordinates_type (alpha) | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therfore defines the dimension of the space. The meaning of these predefined integer constants can be found in the documentation of the grid service library | |
edge_sources.source[:].ggd[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier) | ||
edge_sources.source[:].ggd[:].grid.space[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
edge_sources.source[:].ggd[:].grid.space[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_sources.source[:].ggd[:].grid.space[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
edge_sources.source[:].ggd[:].grid.space[:].objects_per_dimension (alpha) | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
edge_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
edge_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary (alpha) | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
edge_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].index (alpha) | INT_0D | Index of this (n-1)-dimensional boundary object | ||
edge_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].neighbours (alpha) | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
edge_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].geometry (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. |
edge_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].measure (alpha) | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
edge_sources.source[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].nodes (alpha) | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
edge_sources.source[:].ggd[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Source terms related to the different ion species | |
edge_sources.source[:].ggd[:].ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_sources.source[:].ggd[:].ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_sources.source[:].ggd[:].ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_sources.source[:].ggd[:].ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_sources.source[:].ggd[:].ion[:].energy (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Source term for the ion energy transport equation, on various grid subsets |
edge_sources.source[:].ggd[:].ion[:].energy[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].energy[:].values, | FLT_2D (uncertain) | W.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].energy[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].energy[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].ion[:].energy[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
edge_sources.source[:].ggd[:].ion[:].momentum (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Source term for momentum equations (sum over states when multiple states are considered), on various grid subsets |
edge_sources.source[:].ggd[:].ion[:].momentum[:].diamagnetic (alpha) | [edge_sources.source[:].ggd[:].ion[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].momentum[:].diamagnetic_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].momentum[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].momentum[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].ion[:].momentum[:].parallel (alpha) | [edge_sources.source[:].ggd[:].ion[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].momentum[:].parallel_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].momentum[:].poloidal (alpha) | [edge_sources.source[:].ggd[:].ion[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].momentum[:].poloidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].momentum[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].momentum[:].radial_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].momentum[:].toroidal (alpha) | [edge_sources.source[:].ggd[:].ion[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].momentum[:].toroidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_sources.source[:].ggd[:].ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
edge_sources.source[:].ggd[:].ion[:].particles (alpha) | [1...N] | STRUCT_ARRAY | s^-1.m^-3 | Source term for ion density equation, on various grid subsets |
edge_sources.source[:].ggd[:].ion[:].particles[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].particles[:].values, | FLT_2D (uncertain) | s^-1.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].particles[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].particles[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].ion[:].particles[:].values (alpha) | [1...N] | FLT_1D (uncertain) | s^-1.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state (alpha) | [1...N] | STRUCT_ARRAY | Source terms related to the different charge states of the species (ionisation, energy, excitation, ...) | |
edge_sources.source[:].ggd[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_sources.source[:].ggd[:].ion[:].state[:].energy (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Source terms for the charge state energy transport equation |
edge_sources.source[:].ggd[:].ion[:].state[:].energy[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].energy[:].values, | FLT_2D (uncertain) | W.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].state[:].energy[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].state[:].energy[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].ion[:].state[:].energy[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
edge_sources.source[:].ggd[:].ion[:].state[:].momentum (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Source term for momentum equations, on various grid subsets |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].diamagnetic (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].diamagnetic_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].parallel (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].parallel_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].poloidal (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].poloidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].toroidal (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].toroidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].state[:].particles (alpha) | [1...N] | STRUCT_ARRAY | s^-1.m^-3 | Source term for the charge state density transport equation |
edge_sources.source[:].ggd[:].ion[:].state[:].particles[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].ion[:].state[:].particles[:].values, | FLT_2D (uncertain) | s^-1.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].ion[:].state[:].particles[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].state[:].particles[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].ion[:].state[:].particles[:].values (alpha) | [1...N] | FLT_1D (uncertain) | s^-1.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_sources.source[:].ggd[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_sources.source[:].ggd[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle | |
edge_sources.source[:].ggd[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
edge_sources.source[:].ggd[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
edge_sources.source[:].ggd[:].momentum (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Source term for total momentum equations, on various grid subsets |
edge_sources.source[:].ggd[:].momentum[:].diamagnetic (alpha) | [edge_sources.source[:].ggd[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].momentum[:].diamagnetic_coefficients (alpha) | [edge_sources.source[:].ggd[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].momentum[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].momentum[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].momentum[:].parallel (alpha) | [edge_sources.source[:].ggd[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].momentum[:].parallel_coefficients (alpha) | [edge_sources.source[:].ggd[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].momentum[:].poloidal (alpha) | [edge_sources.source[:].ggd[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].momentum[:].poloidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].momentum[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].momentum[:].radial_coefficients (alpha) | [edge_sources.source[:].ggd[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].momentum[:].toroidal (alpha) | [edge_sources.source[:].ggd[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].momentum[:].toroidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral (alpha) | [1...N] | STRUCT_ARRAY | Source terms related to the different neutral species | |
edge_sources.source[:].ggd[:].neutral[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_sources.source[:].ggd[:].neutral[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_sources.source[:].ggd[:].neutral[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_sources.source[:].ggd[:].neutral[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_sources.source[:].ggd[:].neutral[:].energy (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Source term for the ion energy transport equation, on various grid subsets |
edge_sources.source[:].ggd[:].neutral[:].energy[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].energy[:].values, | FLT_2D (uncertain) | W.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].energy[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].energy[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].neutral[:].energy[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].ion_index (alpha) | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
edge_sources.source[:].ggd[:].neutral[:].label (alpha) | STR_0D | String identifying neutral (e.g. H, D, T, He, C, ...) | ||
edge_sources.source[:].ggd[:].neutral[:].momentum (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Source term for momentum equations (sum over states when multiple states are considered), on various grid subsets |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].diamagnetic (alpha) | [edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].diamagnetic_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].momentum[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].neutral[:].momentum[:].parallel (alpha) | [edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].parallel_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].poloidal (alpha) | [edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].poloidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].toroidal (alpha) | [edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].toroidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_sources.source[:].ggd[:].neutral[:].particles (alpha) | [1...N] | STRUCT_ARRAY | s^-1.m^-3 | Source term for ion density equation, on various grid subsets |
edge_sources.source[:].ggd[:].neutral[:].particles[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].particles[:].values, | FLT_2D (uncertain) | s^-1.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].particles[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].particles[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].neutral[:].particles[:].values (alpha) | [1...N] | FLT_1D (uncertain) | s^-1.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state (alpha) | [1...N] | STRUCT_ARRAY | Source terms related to the different charge states of the species (energy, excitation, ...) | |
edge_sources.source[:].ggd[:].neutral[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].energy (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Source terms for the charge state energy transport equation |
edge_sources.source[:].ggd[:].neutral[:].state[:].energy[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].energy[:].values, | FLT_2D (uncertain) | W.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].state[:].energy[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].energy[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].energy[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state[:].label (alpha) | STR_0D | String identifying state | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Source term for momentum equations, on various grid subsets |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].diamagnetic (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].diamagnetic_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].parallel (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].parallel_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].poloidal (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].poloidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].toroidal (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].toroidal_coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].state[:].neutral_type (alpha) | STRUCTURE | Neutral type, in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].neutral_type.description (alpha) | STR_0D | Verbose description | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].neutral_type.name (alpha) | STR_0D | Short string identifier | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].particles (alpha) | [1...N] | STRUCT_ARRAY | s^-1.m^-3 | Source term for the charge state density transport equation |
edge_sources.source[:].ggd[:].neutral[:].state[:].particles[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].neutral[:].state[:].particles[:].values, | FLT_2D (uncertain) | s^-1.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].neutral[:].state[:].particles[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].particles[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].particles[:].values (alpha) | [1...N] | FLT_1D (uncertain) | s^-1.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_sources.source[:].ggd[:].neutral[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_sources.source[:].ggd[:].time (alpha) | FLT_0D | s | Time | |
edge_sources.source[:].ggd[:].total_ion_energy (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Source term for the total (summed over ion species) energy equation, on various grid subsets |
edge_sources.source[:].ggd[:].total_ion_energy[:].coefficients (alpha) | [edge_sources.source[:].ggd[:].total_ion_energy[:].values, | FLT_2D (uncertain) | W.m^-3 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_sources.source[:].ggd[:].total_ion_energy[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].total_ion_energy[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_sources.source[:].ggd[:].total_ion_energy[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].identifier (alpha) | STRUCTURE | Source term identifier | ||
edge_sources.source[:].identifier.description (alpha) | STR_0D | Verbose description | ||
edge_sources.source[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_sources.source[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
edge_sources.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
edge_transport (alpha) | Edge plasma transport. Energy terms correspond to the full kinetic energy equation (i.e. the energy flux takes into account the energy transported by the particle flux) | |||
edge_transport.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
edge_transport.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_transport.code.name (alpha) | STR_0D | Name of software generating IDS | ||
edge_transport.code.output_flag (alpha) | [edge_transport.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
edge_transport.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
edge_transport.code.repository (alpha) | STR_0D | URL of software repository | ||
edge_transport.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_transport.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
edge_transport.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
edge_transport.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
edge_transport.ids_properties.occurrence | INT_0D | |||
edge_transport.model (alpha) | [1...N_Models] | STRUCT_ARRAY | Transport is described by a combination of various transport models | |
edge_transport.model[:].flux_multiplier (alpha) | FLT_0D (uncertain) | - | Multiplier applied to the particule flux when adding its contribution in the expression of the heat flux : can be 0, 3/2 or 5/2 | |
edge_transport.model[:].ggd (alpha) | [edge_transport.model[:].ggd[:].time] | STRUCT_ARRAY | Transport coefficients represented using the general grid description, for various time slices | |
edge_transport.model[:].ggd[:].conductivity (alpha) | [1...N] | STRUCT_ARRAY | ohm^-1.m^-1 | Conductivity, on various grid subsets |
edge_transport.model[:].ggd[:].conductivity[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].conductivity[:].radial] | FLT_1D (uncertain) | ohm^-1.m^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].conductivity[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].conductivity[:].radial, | FLT_2D (uncertain) | ohm^-1.m^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].conductivity[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].conductivity[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].conductivity[:].parallel (alpha) | [edge_transport.model[:].ggd[:].conductivity[:].radial] | FLT_1D (uncertain) | ohm^-1.m^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].conductivity[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].conductivity[:].radial, | FLT_2D (uncertain) | ohm^-1.m^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].conductivity[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].conductivity[:].radial] | FLT_1D (uncertain) | ohm^-1.m^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].conductivity[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].conductivity[:].radial, | FLT_2D (uncertain) | ohm^-1.m^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].conductivity[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | ohm^-1.m^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].conductivity[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].conductivity[:].radial, | FLT_2D (uncertain) | ohm^-1.m^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].conductivity[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].conductivity[:].radial] | FLT_1D (uncertain) | ohm^-1.m^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].conductivity[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].conductivity[:].radial, | FLT_2D (uncertain) | ohm^-1.m^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].electrons (alpha) | STRUCTURE | Transport quantities related to the electrons | ||
edge_transport.model[:].ggd[:].electrons.energy (alpha) | STRUCTURE | Transport quantities for the electron energy equation | ||
edge_transport.model[:].ggd[:].electrons.energy.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].electrons.energy.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].electrons.energy.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].electrons.energy.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].electrons.energy.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].electrons.energy.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].electrons.energy.flux (alpha) | [1...N] | STRUCT_ARRAY | W.m^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].electrons.energy.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].electrons.energy.flux[:].values, | FLT_2D (uncertain) | W.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].electrons.energy.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].electrons.energy.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].electrons.energy.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-2 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].electrons.energy.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].electrons.energy.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].electrons.energy.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].electrons.energy.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].electrons.energy.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].electrons.energy.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].electrons.energy.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].electrons.energy.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].electrons.energy.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].electrons.energy.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].electrons.energy.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].electrons.energy.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].electrons.particles (alpha) | STRUCTURE | Transport quantities for the electron density equation | ||
edge_transport.model[:].ggd[:].electrons.particles.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].electrons.particles.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].electrons.particles.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].electrons.particles.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].electrons.particles.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].electrons.particles.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].electrons.particles.flux (alpha) | [1...N] | STRUCT_ARRAY | m^-2.s^-1 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].electrons.particles.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].electrons.particles.flux[:].values, | FLT_2D (uncertain) | m^-2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].electrons.particles.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].electrons.particles.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].electrons.particles.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].electrons.particles.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].electrons.particles.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].electrons.particles.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].electrons.particles.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].electrons.particles.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].electrons.particles.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].electrons.particles.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].electrons.particles.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].electrons.particles.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].electrons.particles.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].electrons.particles.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].electrons.particles.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].grid (alpha) | STRUCTURE | Grid description | ||
edge_transport.model[:].ggd[:].grid.grid_subset (alpha) | [1...N] | STRUCT_ARRAY | Grid subsets | |
edge_transport.model[:].ggd[:].grid.grid_subset[:].base (alpha) | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
edge_transport.model[:].ggd[:].grid.grid_subset[:].base[:].jacobian (alpha) | [edge_transport.model[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_transport.model[:].ggd[:].grid.grid_subset[:].base[:].tensor_contravariant (alpha) | [edge_transport.model[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_transport.model[:].ggd[:].grid.grid_subset[:].base[:].tensor_covariant (alpha) | [edge_transport.model[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_transport.model[:].ggd[:].grid.grid_subset[:].dimension (alpha) | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
edge_transport.model[:].ggd[:].grid.grid_subset[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
edge_transport.model[:].ggd[:].grid.grid_subset[:].element[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
edge_transport.model[:].ggd[:].grid.grid_subset[:].element[:].object[:].dimension (alpha) | INT_0D | Dimension of the object | ||
edge_transport.model[:].ggd[:].grid.grid_subset[:].element[:].object[:].index (alpha) | INT_0D | Object index | ||
edge_transport.model[:].ggd[:].grid.grid_subset[:].element[:].object[:].space (alpha) | INT_0D | Index of the space from which that object is taken | ||
edge_transport.model[:].ggd[:].grid.grid_subset[:].identifier (alpha) | STRUCTURE | Grid subset identifier | ||
edge_transport.model[:].ggd[:].grid.grid_subset[:].identifier.description (alpha) | STR_0D | Verbose description | ||
edge_transport.model[:].ggd[:].grid.grid_subset[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_transport.model[:].ggd[:].grid.grid_subset[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
edge_transport.model[:].ggd[:].grid.grid_subset[:].metric (alpha) | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
edge_transport.model[:].ggd[:].grid.grid_subset[:].metric.jacobian (alpha) | [edge_transport.model[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_transport.model[:].ggd[:].grid.grid_subset[:].metric.tensor_contravariant (alpha) | [edge_transport.model[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_transport.model[:].ggd[:].grid.grid_subset[:].metric.tensor_covariant (alpha) | [edge_transport.model[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_transport.model[:].ggd[:].grid.identifier (alpha) | STRUCTURE | Grid identifier | ||
edge_transport.model[:].ggd[:].grid.identifier.description (alpha) | STR_0D | Verbose description | ||
edge_transport.model[:].ggd[:].grid.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_transport.model[:].ggd[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
edge_transport.model[:].ggd[:].grid.space (alpha) | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
edge_transport.model[:].ggd[:].grid.space[:].coordinates_type (alpha) | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therfore defines the dimension of the space. The meaning of these predefined integer constants can be found in the documentation of the grid service library | |
edge_transport.model[:].ggd[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier) | ||
edge_transport.model[:].ggd[:].grid.space[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
edge_transport.model[:].ggd[:].grid.space[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_transport.model[:].ggd[:].grid.space[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
edge_transport.model[:].ggd[:].grid.space[:].objects_per_dimension (alpha) | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
edge_transport.model[:].ggd[:].grid.space[:].objects_per_dimension[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
edge_transport.model[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary (alpha) | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
edge_transport.model[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].index (alpha) | INT_0D | Index of this (n-1)-dimensional boundary object | ||
edge_transport.model[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].neighbours (alpha) | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
edge_transport.model[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].geometry (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. |
edge_transport.model[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].measure (alpha) | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
edge_transport.model[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].nodes (alpha) | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
edge_transport.model[:].ggd[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Transport coefficients related to the various ion and neutral species | |
edge_transport.model[:].ggd[:].ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_transport.model[:].ggd[:].ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_transport.model[:].ggd[:].ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_transport.model[:].ggd[:].ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_transport.model[:].ggd[:].ion[:].energy (alpha) | STRUCTURE | Transport coefficients related to the ion energy equation | ||
edge_transport.model[:].ggd[:].ion[:].energy.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].energy.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].energy.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].energy.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].energy.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].energy.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].energy.flux (alpha) | [1...N] | STRUCT_ARRAY | W.m^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].energy.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].energy.flux[:].values, | FLT_2D (uncertain) | W.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].energy.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].energy.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].energy.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-2 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].energy.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].energy.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].energy.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].energy.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].energy.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].energy.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].energy.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].energy.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].energy.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].energy.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].energy.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].energy.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
edge_transport.model[:].ggd[:].ion[:].momentum (alpha) | STRUCTURE | Transport coefficients for the ion momentum equations | ||
edge_transport.model[:].ggd[:].ion[:].momentum.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].parallel (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.d[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].parallel (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].parallel (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | - | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].parallel (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].momentum.v[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_transport.model[:].ggd[:].ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
edge_transport.model[:].ggd[:].ion[:].particles (alpha) | STRUCTURE | Transport related to the ion density equation | ||
edge_transport.model[:].ggd[:].ion[:].particles.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].particles.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].particles.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].particles.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].particles.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].particles.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].particles.flux (alpha) | [1...N] | STRUCT_ARRAY | m^-2.s^-1 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].particles.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].particles.flux[:].values, | FLT_2D (uncertain) | m^-2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].particles.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].particles.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].particles.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].particles.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].particles.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].particles.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].particles.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].particles.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].particles.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].particles.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].particles.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].particles.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].particles.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].particles.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].particles.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state (alpha) | [1...N] | STRUCT_ARRAY | Transport coefficients related to the different states of the species | |
edge_transport.model[:].ggd[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy (alpha) | STRUCTURE | Transport quantities related to the energy equation of the charge state considered | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].energy.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux (alpha) | [1...N] | STRUCT_ARRAY | W.m^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux[:].values, | FLT_2D (uncertain) | W.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-2 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].energy.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].energy.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].energy.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum (alpha) | STRUCTURE | Transport coefficients related to the momentum equations of the charge state considered | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].parallel (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].parallel (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].parallel (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | - | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].parallel (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].particles (alpha) | STRUCTURE | Transport quantities related to density equation of the charge state considered (thermal+non-thermal) | ||
edge_transport.model[:].ggd[:].ion[:].state[:].particles.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].particles.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].particles.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].particles.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux (alpha) | [1...N] | STRUCT_ARRAY | m^-2.s^-1 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux[:].values, | FLT_2D (uncertain) | m^-2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].particles.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].ion[:].state[:].particles.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].ion[:].state[:].particles.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].ion[:].state[:].particles.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].ion[:].state[:].particles.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_transport.model[:].ggd[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_transport.model[:].ggd[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle | |
edge_transport.model[:].ggd[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
edge_transport.model[:].ggd[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
edge_transport.model[:].ggd[:].momentum (alpha) | STRUCTURE | Transport coefficients for total momentum equation | ||
edge_transport.model[:].ggd[:].momentum.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].momentum.d[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.d[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].momentum.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].momentum.d[:].parallel (alpha) | [edge_transport.model[:].ggd[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.d[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.d[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.d[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.d[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.d[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.d[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.d[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].momentum.flux[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].momentum.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].momentum.flux[:].parallel (alpha) | [edge_transport.model[:].ggd[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].parallel (alpha) | [edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | - | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.flux_limiter[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].momentum.v[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.v[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].momentum.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].momentum.v[:].parallel (alpha) | [edge_transport.model[:].ggd[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.v[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.v[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.v[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.v[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.v[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].momentum.v[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].momentum.v[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral (alpha) | [1...N] | STRUCT_ARRAY | Transport coefficients related to the various ion and neutral species | |
edge_transport.model[:].ggd[:].neutral[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_transport.model[:].ggd[:].neutral[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_transport.model[:].ggd[:].neutral[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_transport.model[:].ggd[:].neutral[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_transport.model[:].ggd[:].neutral[:].energy (alpha) | STRUCTURE | Transport coefficients related to the ion energy equation | ||
edge_transport.model[:].ggd[:].neutral[:].energy.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].energy.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].energy.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].energy.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].energy.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].energy.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].energy.flux (alpha) | [1...N] | STRUCT_ARRAY | W.m^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].energy.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].energy.flux[:].values, | FLT_2D (uncertain) | W.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].energy.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].energy.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].energy.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-2 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].energy.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].energy.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].energy.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].energy.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].energy.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].energy.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].energy.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].energy.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].energy.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].energy.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].energy.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].energy.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].ion_index (alpha) | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
edge_transport.model[:].ggd[:].neutral[:].label (alpha) | STR_0D | String identifying neutral (e.g. H, D, T, He, C, ...) | ||
edge_transport.model[:].ggd[:].neutral[:].momentum (alpha) | STRUCTURE | Transport coefficients for the ion momentum equations | ||
edge_transport.model[:].ggd[:].neutral[:].momentum.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].parallel (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].parallel (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].parallel (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | - | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].parallel (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
edge_transport.model[:].ggd[:].neutral[:].particles (alpha) | STRUCTURE | Transport related to the ion density equation | ||
edge_transport.model[:].ggd[:].neutral[:].particles.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].particles.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].particles.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].particles.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].particles.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].particles.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].particles.flux (alpha) | [1...N] | STRUCT_ARRAY | m^-2.s^-1 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].particles.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].particles.flux[:].values, | FLT_2D (uncertain) | m^-2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].particles.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].particles.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].particles.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].particles.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].particles.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].particles.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].particles.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].particles.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].particles.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].particles.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].particles.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].particles.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].particles.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].particles.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].particles.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state (alpha) | [1...N] | STRUCT_ARRAY | Transport coefficients related to the different states of the species | |
edge_transport.model[:].ggd[:].neutral[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy (alpha) | STRUCTURE | Transport quantities related to the energy equation of the charge state considered | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].energy.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux (alpha) | [1...N] | STRUCT_ARRAY | W.m^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux[:].values, | FLT_2D (uncertain) | W.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-2 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].energy.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].energy.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].label (alpha) | STR_0D | String identifying state | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum (alpha) | STRUCTURE | Transport coefficients related to the momentum equations of the charge state considered | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].parallel (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial] | FLT_1D (uncertain) | m^2.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.d[:].radial, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux (alpha) | [1...N] | STRUCT_ARRAY | kg.m^-1.s^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].parallel (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux[:].radial, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].parallel (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | - | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial] | FLT_1D (uncertain) | - | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.flux_limiter[:].radial, | FLT_2D (uncertain) | - | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].diamagnetic (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Diamagnetic component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].diamagnetic_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the diamagnetic component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].parallel (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Parallel component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].parallel_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the parallel component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].poloidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Poloidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].poloidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the poloidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | Radial component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the radial component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].toroidal (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial] | FLT_1D (uncertain) | m.s^-1 | Toroidal component, one scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].toroidal_coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].momentum.v[:].radial, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients for the toroidal component, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].neutral_type (alpha) | STRUCTURE | Neutral type, in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].neutral_type.description (alpha) | STR_0D | Verbose description | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].neutral_type.name (alpha) | STR_0D | Short string identifier | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles (alpha) | STRUCTURE | Transport quantities related to density equation of the charge state considered (thermal+non-thermal) | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].particles.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux (alpha) | [1...N] | STRUCT_ARRAY | m^-2.s^-1 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux[:].values, | FLT_2D (uncertain) | m^-2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^-2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].neutral[:].state[:].particles.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].neutral[:].state[:].particles.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].neutral[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_transport.model[:].ggd[:].neutral[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_transport.model[:].ggd[:].time (alpha) | FLT_0D | s | Time | |
edge_transport.model[:].ggd[:].total_ion_energy (alpha) | STRUCTURE | Transport coefficients for the total (summed over ion species) energy equation | ||
edge_transport.model[:].ggd[:].total_ion_energy.d (alpha) | [1...N] | STRUCT_ARRAY | m^2.s^-1 | Effective diffusivity, on various grid subsets |
edge_transport.model[:].ggd[:].total_ion_energy.d[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].total_ion_energy.d[:].values, | FLT_2D (uncertain) | m^2.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].total_ion_energy.d[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].total_ion_energy.d[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].total_ion_energy.d[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m^2.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].total_ion_energy.flux (alpha) | [1...N] | STRUCT_ARRAY | W.m^-2 | Flux, on various grid subsets |
edge_transport.model[:].ggd[:].total_ion_energy.flux[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].total_ion_energy.flux[:].values, | FLT_2D (uncertain) | W.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].total_ion_energy.flux[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].total_ion_energy.flux[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].total_ion_energy.flux[:].values (alpha) | [1...N] | FLT_1D (uncertain) | W.m^-2 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].total_ion_energy.flux_limiter (alpha) | [1...N] | STRUCT_ARRAY | - | Flux limiter coefficient, on various grid subsets |
edge_transport.model[:].ggd[:].total_ion_energy.flux_limiter[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].total_ion_energy.flux_limiter[:].values, | FLT_2D (uncertain) | - | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].total_ion_energy.flux_limiter[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].total_ion_energy.flux_limiter[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].total_ion_energy.flux_limiter[:].values (alpha) | [1...N] | FLT_1D (uncertain) | - | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].ggd[:].total_ion_energy.v (alpha) | [1...N] | STRUCT_ARRAY | m.s^-1 | Effective convection, on various grid subsets |
edge_transport.model[:].ggd[:].total_ion_energy.v[:].coefficients (alpha) | [edge_transport.model[:].ggd[:].total_ion_energy.v[:].values, | FLT_2D (uncertain) | m.s^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
edge_transport.model[:].ggd[:].total_ion_energy.v[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
edge_transport.model[:].ggd[:].total_ion_energy.v[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
edge_transport.model[:].ggd[:].total_ion_energy.v[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m.s^-1 | One scalar value is provided per element in the grid subset. |
edge_transport.model[:].identifier (alpha) | STRUCTURE | Transport model identifier | ||
edge_transport.model[:].identifier.description (alpha) | STR_0D | Verbose description | ||
edge_transport.model[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
edge_transport.model[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
edge_transport.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
em_coupling (alpha) | Description of the axisymmetric mutual electromagnetics; does not include non-axisymmetric coil systems; the convention is Quantity_Sensor_Source | |||
em_coupling.active_coils (alpha) | [pf_active.coil] | STR_1D | List of the names of the active PF+CS coils | |
em_coupling.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
em_coupling.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
em_coupling.code.name (alpha) | STR_0D | Name of software generating IDS | ||
em_coupling.code.output_flag (alpha) | [em_coupling.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
em_coupling.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
em_coupling.code.repository (alpha) | STR_0D | URL of software repository | ||
em_coupling.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
em_coupling.field_probes_active (alpha) | [em_coupling.poloidal_probes, | FLT_2D (uncertain) | T/A | Poloidal field coupling from active coils to poloidal field probes |
em_coupling.field_probes_grid (alpha) | [em_coupling.poloidal_probes, | FLT_2D (uncertain) | T/A | Poloidal field coupling from equilibrium grid to poloidal field probes |
em_coupling.field_probes_passive (alpha) | [em_coupling.poloidal_probes, | FLT_2D (uncertain) | T/A | Poloidal field coupling from passive loops to poloidal field probes |
em_coupling.flux_loops (alpha) | [magnetics.flux_loop] | STR_1D | List of the names of the axisymmetric flux loops | |
em_coupling.grid_points (alpha) | [1...N] | STR_1D | List of the names of the plasma region grid points | |
em_coupling.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
em_coupling.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
em_coupling.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
em_coupling.ids_properties.occurrence | INT_0D | |||
em_coupling.mutual_active_active (alpha) | [em_coupling.active_coils, | FLT_2D (uncertain) | H | Mutual inductance coupling from active coils to active coils |
em_coupling.mutual_grid_active (alpha) | [em_coupling.grid_points, | FLT_2D (uncertain) | H | Mutual inductance coupling from active coils to equilibrium grid |
em_coupling.mutual_grid_grid (alpha) | [em_coupling.grid_points, | FLT_2D (uncertain) | H | Mutual inductance from equilibrium grid to itself |
em_coupling.mutual_grid_passive (alpha) | [em_coupling.grid_points, | FLT_2D (uncertain) | H | Mutual inductance coupling from passive loops to equilibrium grid |
em_coupling.mutual_loops_active (alpha) | [em_coupling.flux_loops, | FLT_2D (uncertain) | H | Mutual inductance coupling from active coils to poloidal flux loops |
em_coupling.mutual_loops_grid (alpha) | [em_coupling.flux_loops, | FLT_2D (uncertain) | H | Mutual inductance from equilibrium grid to poloidal flux loops |
em_coupling.mutual_loops_passive (alpha) | [em_coupling.flux_loops, | FLT_2D (uncertain) | H | Mutual inductance coupling from passive loops to poloidal flux loops |
em_coupling.mutual_passive_active (alpha) | [em_coupling.passive_loops, | FLT_2D (uncertain) | H | Mutual inductance coupling from active coils to passive loops |
em_coupling.mutual_passive_passive (alpha) | [em_coupling.passive_loops, | FLT_2D (uncertain) | H | Mutual inductance coupling from passive loops to passive loops |
em_coupling.passive_loops (alpha) | [pf_passive.loop] | STR_1D | List of the names of the passive loops | |
em_coupling.poloidal_probes (alpha) | [magnetics.bpol_probe] | STR_1D | List of the names of poloidal field probes | |
em_coupling.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
equilibrium | Description of a 2D, axi-symmetric, tokamak equilibrium; result of an equilibrium code. | |||
equilibrium.code | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
equilibrium.code.commit | STR_0D | Unique commit reference of software | ||
equilibrium.code.name | STR_0D | Name of software generating IDS | ||
equilibrium.code.output_flag | [equilibrium.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
equilibrium.code.parameters | STR_0D | List of the code specific parameters in XML format | ||
equilibrium.code.repository | STR_0D | URL of software repository | ||
equilibrium.code.version | STR_0D | Unique version (tag) of software | ||
equilibrium.ids_properties | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
equilibrium.ids_properties.comment | STR_0D | Any comment describing the content of this IDS | ||
equilibrium.ids_properties.homogeneous_time | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
equilibrium.ids_properties.occurrence | INT_0D | |||
equilibrium.time | [1...N] | FLT_1D_TYPE | Generic time [s] | |
equilibrium.time_slice | [equilibrium.time_slice[:].time] | STRUCT_ARRAY | Set of equilibria at various time slices | |
equilibrium.time_slice[:].boundary | STRUCTURE | Description of the plasma boundary | ||
equilibrium.time_slice[:].boundary.active_limiter_point | STRUCTURE | RZ position of the active limiter point (point of the plasma boundary in contact with the limiter) | ||
equilibrium.time_slice[:].boundary.active_limiter_point.r | FLT_0D (uncertain) | m | Major radius | |
equilibrium.time_slice[:].boundary.active_limiter_point.z | FLT_0D (uncertain) | m | Height | |
equilibrium.time_slice[:].boundary.b_flux_pol_norm | FLT_0D (uncertain) | - | Value of the normalised poloidal flux at which the boundary is taken | |
equilibrium.time_slice[:].boundary.elongation | FLT_0D (uncertain) | - | Elongation of the plasma boundary | |
equilibrium.time_slice[:].boundary.elongation_lower | FLT_0D (uncertain) | - | Elongation (lower half w.r.t. geometric axis) of the plasma boundary | |
equilibrium.time_slice[:].boundary.elongation_upper | FLT_0D (uncertain) | - | Elongation (upper half w.r.t. geometric axis) of the plasma boundary | |
equilibrium.time_slice[:].boundary.geometric_axis | STRUCTURE | RZ position of the geometric axis (defined as (Rmin+Rmax) / 2 and (Zmin+Zmax) / 2 of the boundary) | ||
equilibrium.time_slice[:].boundary.geometric_axis.r | FLT_0D (uncertain) | m | Major radius | |
equilibrium.time_slice[:].boundary.geometric_axis.z | FLT_0D (uncertain) | m | Height | |
equilibrium.time_slice[:].boundary.lcfs (obsolescent) | STRUCTURE | RZ description of the plasma boundary | ||
equilibrium.time_slice[:].boundary.lcfs.r (obsolescent) | [1...N] | FLT_1D (uncertain) | m | Major radius |
equilibrium.time_slice[:].boundary.lcfs.z (obsolescent) | [equilibrium.time_slice[:].boundary.lcfs.r] | FLT_1D (uncertain) | m | Height |
equilibrium.time_slice[:].boundary.minor_radius | FLT_0D (uncertain) | m | Minor radius of the plasma boundary (defined as (Rmax-Rmin) / 2 of the boundary) | |
equilibrium.time_slice[:].boundary.outline | STRUCTURE | RZ outline of the plasma boundary | ||
equilibrium.time_slice[:].boundary.outline.r | [1...N] | FLT_1D (uncertain) | m | Major radius |
equilibrium.time_slice[:].boundary.outline.z | [equilibrium.time_slice[:].boundary.outline.r] | FLT_1D (uncertain) | m | Height |
equilibrium.time_slice[:].boundary.strike_point | [1...N] | STRUCT_ARRAY | Array of strike points, for each of them the RZ position is given | |
equilibrium.time_slice[:].boundary.strike_point[:].r | FLT_0D (uncertain) | m | Major radius | |
equilibrium.time_slice[:].boundary.strike_point[:].z | FLT_0D (uncertain) | m | Height | |
equilibrium.time_slice[:].boundary.triangularity | FLT_0D (uncertain) | - | Triangularity of the plasma boundary | |
equilibrium.time_slice[:].boundary.triangularity_lower | FLT_0D (uncertain) | - | Lower triangularity of the plasma boundary | |
equilibrium.time_slice[:].boundary.triangularity_upper | FLT_0D (uncertain) | - | Upper triangularity of the plasma boundary | |
equilibrium.time_slice[:].boundary.type | INT_0D | 0 (limiter) or 1 (diverted) | ||
equilibrium.time_slice[:].boundary.x_point | [1...N] | STRUCT_ARRAY | Array of X-points, for each of them the RZ position is given | |
equilibrium.time_slice[:].boundary.x_point[:].r | FLT_0D (uncertain) | m | Major radius | |
equilibrium.time_slice[:].boundary.x_point[:].z | FLT_0D (uncertain) | m | Height | |
equilibrium.time_slice[:].coordinate_system | STRUCTURE | Flux surface coordinate system on a square grid of flux and poloidal angle | ||
equilibrium.time_slice[:].coordinate_system.g11_contravariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g11, contravariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g11_covariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g11, covariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g12_contravariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g12, contravariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g12_covariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g12, covariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g13_contravariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g13, contravariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g13_covariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g13, covariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g22_contravariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g22, contravariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g22_covariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g22, covariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g23_contravariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g23, contravariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g23_covariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g23, covariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g33_contravariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g33, contravariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.g33_covariant (obsolescent) | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | metric coefficients g33, covariant metric tensor for the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.grid | STRUCTURE | Definition of the 2D grid | ||
equilibrium.time_slice[:].coordinate_system.grid.dim1 | [1...N] | FLT_1D (uncertain) | mixed | First dimension values |
equilibrium.time_slice[:].coordinate_system.grid.dim2 | [1...N] | FLT_1D (uncertain) | mixed | Second dimension values |
equilibrium.time_slice[:].coordinate_system.grid.volume_element | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | m^3 | Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i) dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)] |
equilibrium.time_slice[:].coordinate_system.grid_type | STRUCTURE | Type of coordinate system | ||
equilibrium.time_slice[:].coordinate_system.grid_type.description | STR_0D | Verbose description | ||
equilibrium.time_slice[:].coordinate_system.grid_type.index | INT_0D | Integer identifier (enumeration index within a list) | ||
equilibrium.time_slice[:].coordinate_system.grid_type.name | STR_0D | Short string identifier | ||
equilibrium.time_slice[:].coordinate_system.jacobian | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | mixed | Jacobian of the coordinate system |
equilibrium.time_slice[:].coordinate_system.r | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | m | Values of the major radius on the grid |
equilibrium.time_slice[:].coordinate_system.tensor_contravariant | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_4D (uncertain) | mixed | Contravariant metric tensor on every point of the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.tensor_covariant | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_4D (uncertain) | mixed | Covariant metric tensor on every point of the grid described by grid_type |
equilibrium.time_slice[:].coordinate_system.z | [equilibrium.time_slice[:].coordinate_system.grid.dim1, | FLT_2D (uncertain) | m | Values of the Height on the grid |
equilibrium.time_slice[:].ggd (alpha) | [1...N] | STRUCT_ARRAY | Equilibrium representation using the generic grid description. Multiple GGD representations of the equilibrium can be stored here. | |
equilibrium.time_slice[:].ggd[:].b_field_r (alpha) | [1...N] | STRUCT_ARRAY | T | R component of the poloidal magnetic field, given on various grid subsets |
equilibrium.time_slice[:].ggd[:].b_field_r[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].b_field_r[:].values, | FLT_2D (uncertain) | T | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].b_field_r[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].b_field_r[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].b_field_r[:].values (alpha) | [1...N] | FLT_1D (uncertain) | T | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].ggd[:].b_field_tor (alpha) | [1...N] | STRUCT_ARRAY | T | Toroidal component of the magnetic field, given on various grid subsets |
equilibrium.time_slice[:].ggd[:].b_field_tor[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].b_field_tor[:].values, | FLT_2D (uncertain) | T | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].b_field_tor[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].b_field_tor[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].b_field_tor[:].values (alpha) | [1...N] | FLT_1D (uncertain) | T | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].ggd[:].b_field_z (alpha) | [1...N] | STRUCT_ARRAY | T | Z component of the poloidal magnetic field, given on various grid subsets |
equilibrium.time_slice[:].ggd[:].b_field_z[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].b_field_z[:].values, | FLT_2D (uncertain) | T | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].b_field_z[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].b_field_z[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].b_field_z[:].values (alpha) | [1...N] | FLT_1D (uncertain) | T | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].ggd[:].grid (alpha) | STRUCTURE | Grid description | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset (alpha) | [1...N] | STRUCT_ARRAY | Grid subsets | |
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].base (alpha) | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].base[:].jacobian (alpha) | [equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].base[:].tensor_contravariant (alpha) | [equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].base[:].tensor_covariant (alpha) | [equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].dimension (alpha) | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element[:].object[:].dimension (alpha) | INT_0D | Dimension of the object | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element[:].object[:].index (alpha) | INT_0D | Object index | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element[:].object[:].space (alpha) | INT_0D | Index of the space from which that object is taken | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].identifier (alpha) | STRUCTURE | Grid subset identifier | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].identifier.description (alpha) | STR_0D | Verbose description | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].metric (alpha) | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].metric.jacobian (alpha) | [equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].metric.tensor_contravariant (alpha) | [equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].metric.tensor_covariant (alpha) | [equilibrium.time_slice[:].ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
equilibrium.time_slice[:].ggd[:].grid.identifier (alpha) | STRUCTURE | Grid identifier | ||
equilibrium.time_slice[:].ggd[:].grid.identifier.description (alpha) | STR_0D | Verbose description | ||
equilibrium.time_slice[:].ggd[:].grid.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
equilibrium.time_slice[:].ggd[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
equilibrium.time_slice[:].ggd[:].grid.space (alpha) | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
equilibrium.time_slice[:].ggd[:].grid.space[:].coordinates_type (alpha) | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therfore defines the dimension of the space. The meaning of these predefined integer constants can be found in the documentation of the grid service library | |
equilibrium.time_slice[:].ggd[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier) | ||
equilibrium.time_slice[:].ggd[:].grid.space[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
equilibrium.time_slice[:].ggd[:].grid.space[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
equilibrium.time_slice[:].ggd[:].grid.space[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
equilibrium.time_slice[:].ggd[:].grid.space[:].objects_per_dimension (alpha) | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
equilibrium.time_slice[:].ggd[:].grid.space[:].objects_per_dimension[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
equilibrium.time_slice[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary (alpha) | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
equilibrium.time_slice[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].index (alpha) | INT_0D | Index of this (n-1)-dimensional boundary object | ||
equilibrium.time_slice[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].neighbours (alpha) | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
equilibrium.time_slice[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].geometry (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. |
equilibrium.time_slice[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].measure (alpha) | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
equilibrium.time_slice[:].ggd[:].grid.space[:].objects_per_dimension[:].object[:].nodes (alpha) | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
equilibrium.time_slice[:].ggd[:].j_parallel (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Parallel (to magnetic field) plasma current density, given on various grid subsets |
equilibrium.time_slice[:].ggd[:].j_parallel[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].j_parallel[:].values, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].j_parallel[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].j_parallel[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].j_parallel[:].values (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].ggd[:].j_tor (alpha) | [1...N] | STRUCT_ARRAY | A.m^-2 | Toroidal plasma current density, given on various grid subsets |
equilibrium.time_slice[:].ggd[:].j_tor[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].j_tor[:].values, | FLT_2D (uncertain) | A.m^-2 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].j_tor[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].j_tor[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].j_tor[:].values (alpha) | [1...N] | FLT_1D (uncertain) | A.m^-2 | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].ggd[:].phi (alpha) | [1...N] | STRUCT_ARRAY | Wb | Values of the toroidal flux, given on various grid subsets |
equilibrium.time_slice[:].ggd[:].phi[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].phi[:].values, | FLT_2D (uncertain) | Wb | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].phi[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].phi[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].phi[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Wb | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].ggd[:].psi (alpha) | [1...N] | STRUCT_ARRAY | Wb | Values of the poloidal flux, given on various grid subsets |
equilibrium.time_slice[:].ggd[:].psi[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].psi[:].values, | FLT_2D (uncertain) | Wb | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].psi[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].psi[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].psi[:].values (alpha) | [1...N] | FLT_1D (uncertain) | Wb | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].ggd[:].r (alpha) | [1...N] | STRUCT_ARRAY | m | Values of the major radius on various grid subsets |
equilibrium.time_slice[:].ggd[:].r[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].r[:].values, | FLT_2D (uncertain) | m | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].r[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].r[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].r[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].ggd[:].theta (alpha) | [1...N] | STRUCT_ARRAY | rad | Values of the poloidal angle, given on various grid subsets |
equilibrium.time_slice[:].ggd[:].theta[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].theta[:].values, | FLT_2D (uncertain) | rad | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].theta[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].theta[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].theta[:].values (alpha) | [1...N] | FLT_1D (uncertain) | rad | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].ggd[:].z (alpha) | [1...N] | STRUCT_ARRAY | m | Values of the Height on various grid subsets |
equilibrium.time_slice[:].ggd[:].z[:].coefficients (alpha) | [equilibrium.time_slice[:].ggd[:].z[:].values, | FLT_2D (uncertain) | m | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
equilibrium.time_slice[:].ggd[:].z[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
equilibrium.time_slice[:].ggd[:].z[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
equilibrium.time_slice[:].ggd[:].z[:].values (alpha) | [1...N] | FLT_1D (uncertain) | m | One scalar value is provided per element in the grid subset. |
equilibrium.time_slice[:].global_quantities | STRUCTURE | 0D parameters of the equilibrium | ||
equilibrium.time_slice[:].global_quantities.area | FLT_0D (uncertain) | m^2 | Area of the LCFS poloidal cross section | |
equilibrium.time_slice[:].global_quantities.beta_normal | FLT_0D (uncertain) | - | Normalised toroidal beta, defined as 100 * beta_tor * a[m] * B0 [T] / ip [MA] | |
equilibrium.time_slice[:].global_quantities.beta_pol | FLT_0D (uncertain) | - | Poloidal beta. Defined as betap = 4 int(p dV) / [R_0 * mu_0 * Ip^2] | |
equilibrium.time_slice[:].global_quantities.beta_tor | FLT_0D (uncertain) | - | Toroidal beta, defined as the volume-averaged total perpendicular pressure divided by (B0^2/(2*mu0)), i.e. beta_toroidal = 2 mu0 int(p dV) / V / B0^2 | |
equilibrium.time_slice[:].global_quantities.ip | FLT_0D (uncertain) | A | Plasma current. Positive sign means anti-clockwise when viewed from above. | |
equilibrium.time_slice[:].global_quantities.length_pol | FLT_0D (uncertain) | m | Poloidal length of the magnetic surface | |
equilibrium.time_slice[:].global_quantities.li_3 | FLT_0D (uncertain) | - | Internal inductance | |
equilibrium.time_slice[:].global_quantities.magnetic_axis | STRUCTURE | Magnetic axis position and toroidal field | ||
equilibrium.time_slice[:].global_quantities.magnetic_axis.b_field_tor | FLT_0D (uncertain) | T | Total toroidal magnetic field at the magnetic axis | |
equilibrium.time_slice[:].global_quantities.magnetic_axis.b_tor (obsolescent) | FLT_0D (uncertain) | T | Total toroidal magnetic field at the magnetic axis | |
equilibrium.time_slice[:].global_quantities.magnetic_axis.r | FLT_0D (uncertain) | m | Major radius of the magnetic axis | |
equilibrium.time_slice[:].global_quantities.magnetic_axis.z | FLT_0D (uncertain) | m | Height of the magnetic axis | |
equilibrium.time_slice[:].global_quantities.psi_axis | FLT_0D (uncertain) | Wb | Poloidal flux at the magnetic axis | |
equilibrium.time_slice[:].global_quantities.psi_boundary | FLT_0D (uncertain) | Wb | Poloidal flux at the selected plasma boundary | |
equilibrium.time_slice[:].global_quantities.q_95 | FLT_0D (uncertain) | - | q at the 95% poloidal flux surface | |
equilibrium.time_slice[:].global_quantities.q_axis | FLT_0D (uncertain) | - | q at the magnetic axis | |
equilibrium.time_slice[:].global_quantities.q_min | STRUCTURE | Minimum q value and position | ||
equilibrium.time_slice[:].global_quantities.q_min.rho_tor_norm | FLT_0D (uncertain) | - | Minimum q position in normalised toroidal flux coordinate | |
equilibrium.time_slice[:].global_quantities.q_min.value | FLT_0D (uncertain) | - | Minimum q value | |
equilibrium.time_slice[:].global_quantities.surface | FLT_0D (uncertain) | m^2 | Surface area of the toroidal flux surface | |
equilibrium.time_slice[:].global_quantities.volume | FLT_0D (uncertain) | m^3 | Total plasma volume | |
equilibrium.time_slice[:].global_quantities.w_mhd | FLT_0D (uncertain) | J | Plasma energy content = 3/2 * int(p,dV) with p being the total pressure (thermal + fast particles) [J]. Time-dependent; Scalar | |
equilibrium.time_slice[:].profiles_1d | STRUCTURE | Equilibrium profiles (1D radial grid) as a function of the poloidal flux | ||
equilibrium.time_slice[:].profiles_1d.area | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
equilibrium.time_slice[:].profiles_1d.b_average (obsolescent) | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T | Flux surface averaged B |
equilibrium.time_slice[:].profiles_1d.b_field_average | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T | Flux surface averaged B |
equilibrium.time_slice[:].profiles_1d.b_field_max | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T | Maximum(B) on the flux surface |
equilibrium.time_slice[:].profiles_1d.b_field_min | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T | Minimum(B) on the flux surface |
equilibrium.time_slice[:].profiles_1d.b_max (obsolescent) | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T | Maximum(B) on the flux surface |
equilibrium.time_slice[:].profiles_1d.b_min (obsolescent) | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T | Minimum(B) on the flux surface |
equilibrium.time_slice[:].profiles_1d.beta_pol | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Poloidal beta profile. Defined as betap = 4 int(p dV) / [R_0 * mu_0 * Ip^2] |
equilibrium.time_slice[:].profiles_1d.darea_dpsi | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m^2.Wb^-1 | Radial derivative of the cross-sectional area of the flux surface with respect to psi |
equilibrium.time_slice[:].profiles_1d.darea_drho_tor | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m | Radial derivative of the cross-sectional area of the flux surface with respect to rho_tor |
equilibrium.time_slice[:].profiles_1d.dpressure_dpsi | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | Pa.Wb^-1 | Derivative of pressure w.r.t. psi |
equilibrium.time_slice[:].profiles_1d.dpsi_drho_tor | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | Wb/m | Derivative of Psi with respect to Rho_Tor |
equilibrium.time_slice[:].profiles_1d.dvolume_dpsi | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m^3.Wb^-1 | Radial derivative of the volume enclosed in the flux surface with respect to Psi |
equilibrium.time_slice[:].profiles_1d.dvolume_drho_tor | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m^2 | Radial derivative of the volume enclosed in the flux surface with respect to Rho_Tor |
equilibrium.time_slice[:].profiles_1d.elongation | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Elongation |
equilibrium.time_slice[:].profiles_1d.f | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T.m | Diamagnetic function (F=R B_Phi) |
equilibrium.time_slice[:].profiles_1d.f_df_dpsi | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T^2.m^2/Wb | Derivative of F w.r.t. Psi, multiplied with F |
equilibrium.time_slice[:].profiles_1d.gm1 | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m^-2 | Flux surface averaged 1/R^2 |
equilibrium.time_slice[:].profiles_1d.gm2 | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m^-2 | Flux surface averaged grad_rho^2/R^2 |
equilibrium.time_slice[:].profiles_1d.gm3 | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Flux surface averaged grad_rho^2 |
equilibrium.time_slice[:].profiles_1d.gm4 | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T^-2 | Flux surface averaged 1/B^2 |
equilibrium.time_slice[:].profiles_1d.gm5 | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T^2 | Flux surface averaged B^2 |
equilibrium.time_slice[:].profiles_1d.gm6 | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | T^-2 | Flux surface averaged grad_rho^2/B^2 |
equilibrium.time_slice[:].profiles_1d.gm7 | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Flux surface averaged grad_rho |
equilibrium.time_slice[:].profiles_1d.gm8 | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m | Flux surface averaged R |
equilibrium.time_slice[:].profiles_1d.gm9 | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m^-1 | Flux surface averaged 1/R |
equilibrium.time_slice[:].profiles_1d.j_parallel | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | A/m^2 | Flux surface averaged parallel current density = average(j.B) / B0, where B0 = Equilibrium/Global/Toroidal_Field/B0 |
equilibrium.time_slice[:].profiles_1d.j_tor | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | A/m^2 | Flux surface averaged toroidal current density = average(j_tor/R) / average(1/R) |
equilibrium.time_slice[:].profiles_1d.magnetic_shear | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor |
equilibrium.time_slice[:].profiles_1d.mass_density | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | kg.m^-3 | Mass density |
equilibrium.time_slice[:].profiles_1d.phi | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | Wb | Toroidal flux |
equilibrium.time_slice[:].profiles_1d.pressure | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | Pa | Pressure |
equilibrium.time_slice[:].profiles_1d.psi | [1...N] | FLT_1D (uncertain) | Wb | Poloidal flux |
equilibrium.time_slice[:].profiles_1d.q | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Safety factor |
equilibrium.time_slice[:].profiles_1d.r_inboard | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m | Radial coordinate (major radius) on the inboard side of the magnetic axis |
equilibrium.time_slice[:].profiles_1d.r_outboard | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m | Radial coordinate (major radius) on the outboard side of the magnetic axis |
equilibrium.time_slice[:].profiles_1d.rho_tor | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m | Toroidal flux coordinate. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
equilibrium.time_slice[:].profiles_1d.rho_tor_norm | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation) |
equilibrium.time_slice[:].profiles_1d.rho_volume_norm | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Normalised square root of enclosed volume (radial coordinate). The normalizing value is the enclosed volume at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation) |
equilibrium.time_slice[:].profiles_1d.surface | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m^2 | Surface area of the toroidal flux surface |
equilibrium.time_slice[:].profiles_1d.trapped_fraction | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Trapped particle fraction |
equilibrium.time_slice[:].profiles_1d.triangularity_lower | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Lower triangularity w.r.t. magnetic axis |
equilibrium.time_slice[:].profiles_1d.triangularity_upper | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | - | Upper triangularity w.r.t. magnetic axis |
equilibrium.time_slice[:].profiles_1d.volume | [equilibrium.time_slice[:].profiles_1d.psi] | FLT_1D (uncertain) | m^3 | Volume enclosed in the flux surface |
equilibrium.time_slice[:].profiles_2d | [1...N] | STRUCT_ARRAY | Equilibrium 2D profiles in the poloidal plane. Multiple 2D representations of the equilibrium can be stored here. | |
equilibrium.time_slice[:].profiles_2d[:].b_field_r | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | T | R component of the poloidal magnetic field |
equilibrium.time_slice[:].profiles_2d[:].b_field_tor | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | T | Toroidal component of the magnetic field |
equilibrium.time_slice[:].profiles_2d[:].b_field_z | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | T | Z component of the poloidal magnetic field |
equilibrium.time_slice[:].profiles_2d[:].b_r (obsolescent) | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | T | R component of the poloidal magnetic field |
equilibrium.time_slice[:].profiles_2d[:].b_tor (obsolescent) | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | T | Toroidal component of the magnetic field |
equilibrium.time_slice[:].profiles_2d[:].b_z (obsolescent) | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | T | Z component of the poloidal magnetic field |
equilibrium.time_slice[:].profiles_2d[:].grid | STRUCTURE | Definition of the 2D grid | ||
equilibrium.time_slice[:].profiles_2d[:].grid.dim1 | [1...N] | FLT_1D (uncertain) | mixed | First dimension values |
equilibrium.time_slice[:].profiles_2d[:].grid.dim2 | [1...N] | FLT_1D (uncertain) | mixed | Second dimension values |
equilibrium.time_slice[:].profiles_2d[:].grid.volume_element | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | m^3 | Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i) dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)] |
equilibrium.time_slice[:].profiles_2d[:].grid_type | STRUCTURE | Selection of one of a set of grid types | ||
equilibrium.time_slice[:].profiles_2d[:].grid_type.description | STR_0D | Verbose description | ||
equilibrium.time_slice[:].profiles_2d[:].grid_type.index | INT_0D | Integer identifier (enumeration index within a list) | ||
equilibrium.time_slice[:].profiles_2d[:].grid_type.name | STR_0D | Short string identifier | ||
equilibrium.time_slice[:].profiles_2d[:].j_parallel | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | A.m^-2 | Parallel (to magnetic field) plasma current density |
equilibrium.time_slice[:].profiles_2d[:].j_tor | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | A.m^-2 | Toroidal plasma current density |
equilibrium.time_slice[:].profiles_2d[:].phi | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | Wb | Toroidal flux |
equilibrium.time_slice[:].profiles_2d[:].psi | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | Wb | Values of the poloidal flux at the grid in the poloidal plane |
equilibrium.time_slice[:].profiles_2d[:].r | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | m | Values of the major radius on the grid |
equilibrium.time_slice[:].profiles_2d[:].theta | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | rad | Values of the poloidal angle on the grid |
equilibrium.time_slice[:].profiles_2d[:].z | [equilibrium.time_slice[:].profiles_2d[:].grid.dim1, | FLT_2D (uncertain) | m | Values of the Height on the grid |
equilibrium.time_slice[:].time | FLT_0D | s | Time | |
equilibrium.vacuum_toroidal_field | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities) | ||
equilibrium.vacuum_toroidal_field.b0 | [equilibrium.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
equilibrium.vacuum_toroidal_field.r0 | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
ic_antennas (alpha) | Antenna systems for heating and current drive in the ion cylcotron (IC) frequencies. | |||
ic_antennas.antenna (alpha) | [1...N] | STRUCT_ARRAY | Set of Ion Cyclotron antennas | |
ic_antennas.antenna[:].frequency (alpha) | STRUCTURE | Frequency | ||
ic_antennas.antenna[:].frequency.data (alpha) | [ic_antennas.antenna[:].frequency.time] | FLT_1D (uncertain) | Hz | Frequency |
ic_antennas.antenna[:].frequency.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ic_antennas.antenna[:].name (alpha) | STR_0D | Name of the antenna | ||
ic_antennas.antenna[:].power (alpha) | STRUCTURE | Power | ||
ic_antennas.antenna[:].power.data (alpha) | [ic_antennas.antenna[:].power.time] | FLT_1D (uncertain) | W | Power |
ic_antennas.antenna[:].power.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ic_antennas.antenna[:].strap (alpha) | [1...N] | STRUCT_ARRAY | Properties of IC antenna straps | |
ic_antennas.antenna[:].strap[:].current (alpha) | STRUCTURE | Root mean square current flowing along the strap | ||
ic_antennas.antenna[:].strap[:].current.data (alpha) | [ic_antennas.antenna[:].strap[:].current.time] | FLT_1D (uncertain) | A | Root mean square current flowing along the strap |
ic_antennas.antenna[:].strap[:].current.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ic_antennas.antenna[:].strap[:].distance_to_conductor (alpha) | FLT_0D (uncertain) | m | Distance to conducting wall or other conductor behind the antenna strap | |
ic_antennas.antenna[:].strap[:].geometry (alpha) | STRUCTURE | Cross-sectional shape of the strap | ||
ic_antennas.antenna[:].strap[:].geometry.geometry_type (alpha) | INT_0D | Type used to describe the element shape (1:'outline', 2:'rectangle', 3:'oblique') | ||
ic_antennas.antenna[:].strap[:].geometry.oblique (alpha) | STRUCTURE | Trapezoidal description of the element | ||
ic_antennas.antenna[:].strap[:].geometry.oblique.alpha (alpha) | FLT_0D (uncertain) | m | Inclination of first angle TBD | |
ic_antennas.antenna[:].strap[:].geometry.oblique.beta (alpha) | FLT_0D (uncertain) | m | Inclination of second angle TBD | |
ic_antennas.antenna[:].strap[:].geometry.oblique.length (alpha) | FLT_0D (uncertain) | m | Length | |
ic_antennas.antenna[:].strap[:].geometry.oblique.r (alpha) | FLT_0D (uncertain) | m | Geometric centre R | |
ic_antennas.antenna[:].strap[:].geometry.oblique.thickness (alpha) | FLT_0D (uncertain) | m | Thickness | |
ic_antennas.antenna[:].strap[:].geometry.oblique.z (alpha) | FLT_0D (uncertain) | m | Geometric centre Z | |
ic_antennas.antenna[:].strap[:].geometry.outline (alpha) | STRUCTURE | Irregular outline of the element | ||
ic_antennas.antenna[:].strap[:].geometry.outline.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
ic_antennas.antenna[:].strap[:].geometry.outline.z (alpha) | [ic_antennas.antenna[:].strap[:].geometry.outline.r] | FLT_1D (uncertain) | m | Height |
ic_antennas.antenna[:].strap[:].geometry.rectangle (alpha) | STRUCTURE | Rectangular description of the element | ||
ic_antennas.antenna[:].strap[:].geometry.rectangle.height (alpha) | FLT_0D (uncertain) | m | Vertical full height | |
ic_antennas.antenna[:].strap[:].geometry.rectangle.r (alpha) | FLT_0D (uncertain) | m | Geometric centre R | |
ic_antennas.antenna[:].strap[:].geometry.rectangle.width (alpha) | FLT_0D (uncertain) | m | Horizontal full width | |
ic_antennas.antenna[:].strap[:].geometry.rectangle.z (alpha) | FLT_0D (uncertain) | m | Geometric centre Z | |
ic_antennas.antenna[:].strap[:].outline (alpha) | STRUCTURE | Strap outline | ||
ic_antennas.antenna[:].strap[:].outline.phi (alpha) | [ic_antennas.antenna[:].strap[:].outline.r] | FLT_1D (uncertain) | rad | Toroidal angle |
ic_antennas.antenna[:].strap[:].outline.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
ic_antennas.antenna[:].strap[:].outline.z (alpha) | [ic_antennas.antenna[:].strap[:].outline.r] | FLT_1D (uncertain) | m | Height |
ic_antennas.antenna[:].strap[:].phase (alpha) | STRUCTURE | Phase of the strap current | ||
ic_antennas.antenna[:].strap[:].phase.data (alpha) | [ic_antennas.antenna[:].strap[:].phase.time] | FLT_1D (uncertain) | rad | Phase of the strap current |
ic_antennas.antenna[:].strap[:].phase.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ic_antennas.antenna[:].strap[:].width_tor (alpha) | FLT_0D (uncertain) | m | Width of strap in the toroidal direction | |
ic_antennas.antenna[:].surface_current (alpha) | [ic_antennas.antenna[:].surface_current[:].time] | STRUCT_ARRAY | Description of the IC surface current on the antenna straps and on passive components, for every time slice | |
ic_antennas.antenna[:].surface_current[:].m_pol (alpha) | [1...N] | INT_1D | Poloidal mode numbers, used to describe the spectrum of the antenna current. The poloidal angle is defined from the reference point; the angle at a point (R,Z) is given by atan((Z-Zref)/(R-Rref)), where Rref=reference_point/r and Zref=reference_point/z | |
ic_antennas.antenna[:].surface_current[:].n_tor (alpha) | [1...N] | INT_1D | Toroidal mode numbers, used to describe the spectrum of the antenna current | |
ic_antennas.antenna[:].surface_current[:].spectrum (alpha) | [ic_antennas.antenna[:].surface_current[:].m_pol, | INT_1D | A | Spectrum of the total surface current on the antenna strap and passive components expressed in poloidal and toroidal modes |
ic_antennas.antenna[:].surface_current[:].time (alpha) | FLT_0D | s | Time | |
ic_antennas.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
ic_antennas.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
ic_antennas.code.name (alpha) | STR_0D | Name of software generating IDS | ||
ic_antennas.code.output_flag (alpha) | [ic_antennas.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
ic_antennas.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
ic_antennas.code.repository (alpha) | STR_0D | URL of software repository | ||
ic_antennas.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
ic_antennas.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
ic_antennas.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
ic_antennas.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
ic_antennas.ids_properties.occurrence | INT_0D | |||
ic_antennas.reference_point (alpha) | STRUCTURE | Reference point used to define the poloidal angle, e.g. the geometrical centre of the vacuum vessel. Used to define the poloidal mode numbers under antenna/surface_current | ||
ic_antennas.reference_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
ic_antennas.reference_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
ic_antennas.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
interfero_polarimeter (alpha) | Interfero-polarimeter diagnostic | |||
interfero_polarimeter.channel (alpha) | [1...N] | STRUCT_ARRAY | Set of channels (lines-of-sight) | |
interfero_polarimeter.channel[:].ellipticity (alpha) | STRUCTURE | Ellipticity | ||
interfero_polarimeter.channel[:].ellipticity.data (alpha) | [interfero_polarimeter.channel[:].ellipticity.time] | FLT_1D (uncertain) | - | Ellipticity |
interfero_polarimeter.channel[:].ellipticity.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
interfero_polarimeter.channel[:].ellipticity_initial (alpha) | FLT_0D (uncertain) | m | Initial ellipticity before entering the plasma | |
interfero_polarimeter.channel[:].faraday_angle (alpha) | STRUCTURE | Faraday angle (variation of the Faraday angle induced by crossing the plasma) | ||
interfero_polarimeter.channel[:].faraday_angle.data (alpha) | [interfero_polarimeter.channel[:].faraday_angle.time] | FLT_1D (uncertain) | rad | Faraday angle (variation of the Faraday angle induced by crossing the plasma) |
interfero_polarimeter.channel[:].faraday_angle.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
interfero_polarimeter.channel[:].identifier (alpha) | STR_0D | ID of the channel | ||
interfero_polarimeter.channel[:].line_of_sight (alpha) | STRUCTURE | Description of the line of sight of the channel, defined by two points when the beam is not reflected, a third point is added to define the reflected beam path | ||
interfero_polarimeter.channel[:].line_of_sight.first_point (alpha) | STRUCTURE | Position of the first point | ||
interfero_polarimeter.channel[:].line_of_sight.first_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
interfero_polarimeter.channel[:].line_of_sight.first_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
interfero_polarimeter.channel[:].line_of_sight.first_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
interfero_polarimeter.channel[:].line_of_sight.second_point (alpha) | STRUCTURE | Position of the second point | ||
interfero_polarimeter.channel[:].line_of_sight.second_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
interfero_polarimeter.channel[:].line_of_sight.second_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
interfero_polarimeter.channel[:].line_of_sight.second_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
interfero_polarimeter.channel[:].line_of_sight.third_point (alpha) | STRUCTURE | Position of the third point | ||
interfero_polarimeter.channel[:].line_of_sight.third_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
interfero_polarimeter.channel[:].line_of_sight.third_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
interfero_polarimeter.channel[:].line_of_sight.third_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
interfero_polarimeter.channel[:].n_e_line (alpha) | STRUCTURE | Line integrated density, possibly obtained by a combination of multiple interferometry wavelengths | ||
interfero_polarimeter.channel[:].n_e_line.data (alpha) | [interfero_polarimeter.channel[:].n_e_line.time] | FLT_1D (uncertain) | m^-2 | Line integrated density, possibly obtained by a combination of multiple interferometry wavelengths |
interfero_polarimeter.channel[:].n_e_line.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
interfero_polarimeter.channel[:].name (alpha) | STR_0D | Name of the channel | ||
interfero_polarimeter.channel[:].polarisation_initial (alpha) | FLT_0D (uncertain) | m | Initial polarisation vector before entering the plasma | |
interfero_polarimeter.channel[:].validity (alpha) | INT_0D | Indicator of the validity of the channel for the whole acquisition period (0 means valid, negative values mean non-valid) | ||
interfero_polarimeter.channel[:].validity_timed (alpha) | STRUCTURE | Indicator of the validity of the channel as a function of time (0 means valid, negative values mean non-valid) | ||
interfero_polarimeter.channel[:].validity_timed.data (alpha) | [interfero_polarimeter.channel[:].validity_timed.time] | INT_1D | Indicator of the validity of the channel as a function of time (0 means valid, negative values mean non-valid) | |
interfero_polarimeter.channel[:].validity_timed.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
interfero_polarimeter.channel[:].wavelength_interferometry (alpha) | [1...N] | STRUCT_ARRAY | Set of wavelengths used for interferometry | |
interfero_polarimeter.channel[:].wavelength_interferometry[:].n_e_line (alpha) | STRUCTURE | Line integrated density estimated from this wavelength | ||
interfero_polarimeter.channel[:].wavelength_interferometry[:].n_e_line.data (alpha) | [interfero_polarimeter.channel[:].wavelength_interferometry[:].n_e_line.time] | FLT_1D (uncertain) | m^-2 | Line integrated density estimated from this wavelength |
interfero_polarimeter.channel[:].wavelength_interferometry[:].n_e_line.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
interfero_polarimeter.channel[:].wavelength_interferometry[:].phase (alpha) | STRUCTURE | Phase measured for this wavelength | ||
interfero_polarimeter.channel[:].wavelength_interferometry[:].phase.data (alpha) | [interfero_polarimeter.channel[:].wavelength_interferometry[:].phase.time] | FLT_1D (uncertain) | rad | Phase measured for this wavelength |
interfero_polarimeter.channel[:].wavelength_interferometry[:].phase.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
interfero_polarimeter.channel[:].wavelength_interferometry[:].value (alpha) | FLT_0D (uncertain) | m | Wavelength value | |
interfero_polarimeter.channel[:].wavelength_polarimetry (alpha) | FLT_0D (uncertain) | m | Wavelength used for polarimetry | |
interfero_polarimeter.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
interfero_polarimeter.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
interfero_polarimeter.code.name (alpha) | STR_0D | Name of software generating IDS | ||
interfero_polarimeter.code.output_flag (alpha) | [interfero_polarimeter.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
interfero_polarimeter.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
interfero_polarimeter.code.repository (alpha) | STR_0D | URL of software repository | ||
interfero_polarimeter.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
interfero_polarimeter.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
interfero_polarimeter.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
interfero_polarimeter.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
interfero_polarimeter.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
iron_core (alpha) | Iron core description | |||
iron_core.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
iron_core.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
iron_core.code.name (alpha) | STR_0D | Name of software generating IDS | ||
iron_core.code.output_flag (alpha) | [iron_core.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
iron_core.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
iron_core.code.repository (alpha) | STR_0D | URL of software repository | ||
iron_core.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
iron_core.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
iron_core.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
iron_core.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
iron_core.ids_properties.occurrence | INT_0D | |||
iron_core.segment (alpha) | [1...N] | STRUCT_ARRAY | The iron core is describred as a set of segments | |
iron_core.segment[:].b_field (alpha) | [1...N] | FLT_1D (uncertain) | T | Array of magnetic field values, for each of which the relative permeability is given |
iron_core.segment[:].geometry (alpha) | STRUCTURE | Cross-sectional shape of the segment | ||
iron_core.segment[:].geometry.geometry_type (alpha) | INT_0D | Type used to describe the element shape (1:'outline', 2:'rectangle', 3:'oblique') | ||
iron_core.segment[:].geometry.oblique (alpha) | STRUCTURE | Trapezoidal description of the element | ||
iron_core.segment[:].geometry.oblique.alpha (alpha) | FLT_0D (uncertain) | m | Inclination of first angle TBD | |
iron_core.segment[:].geometry.oblique.beta (alpha) | FLT_0D (uncertain) | m | Inclination of second angle TBD | |
iron_core.segment[:].geometry.oblique.length (alpha) | FLT_0D (uncertain) | m | Length | |
iron_core.segment[:].geometry.oblique.r (alpha) | FLT_0D (uncertain) | m | Geometric centre R | |
iron_core.segment[:].geometry.oblique.thickness (alpha) | FLT_0D (uncertain) | m | Thickness | |
iron_core.segment[:].geometry.oblique.z (alpha) | FLT_0D (uncertain) | m | Geometric centre Z | |
iron_core.segment[:].geometry.outline (alpha) | STRUCTURE | Irregular outline of the element | ||
iron_core.segment[:].geometry.outline.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
iron_core.segment[:].geometry.outline.z (alpha) | [iron_core.segment[:].geometry.outline.r] | FLT_1D (uncertain) | m | Height |
iron_core.segment[:].geometry.rectangle (alpha) | STRUCTURE | Rectangular description of the element | ||
iron_core.segment[:].geometry.rectangle.height (alpha) | FLT_0D (uncertain) | m | Vertical full height | |
iron_core.segment[:].geometry.rectangle.r (alpha) | FLT_0D (uncertain) | m | Geometric centre R | |
iron_core.segment[:].geometry.rectangle.width (alpha) | FLT_0D (uncertain) | m | Horizontal full width | |
iron_core.segment[:].geometry.rectangle.z (alpha) | FLT_0D (uncertain) | m | Geometric centre Z | |
iron_core.segment[:].identifier (alpha) | STR_0D | ID of the segment | ||
iron_core.segment[:].magnetisation_r (alpha) | STRUCTURE | Magnetisation M of the iron segment along the major radius axis, assumed to be constant inside a given iron segment. Reminder : H = 1/mu0 * B - mur * M; | ||
iron_core.segment[:].magnetisation_r.data (alpha) | [iron_core.segment[:].magnetisation_r.time] | FLT_1D (uncertain) | T | Magnetisation M of the iron segment along the major radius axis, assumed to be constant inside a given iron segment. Reminder : H = 1/mu0 * B - mur * M; |
iron_core.segment[:].magnetisation_r.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
iron_core.segment[:].magnetisation_z (alpha) | STRUCTURE | Magnetisation M of the iron segment along the vertical axis, assumed to be constant inside a given iron segment. Reminder : H = 1/mu0 * B - mur * M; | ||
iron_core.segment[:].magnetisation_z.data (alpha) | [iron_core.segment[:].magnetisation_z.time] | FLT_1D (uncertain) | T | Magnetisation M of the iron segment along the vertical axis, assumed to be constant inside a given iron segment. Reminder : H = 1/mu0 * B - mur * M; |
iron_core.segment[:].magnetisation_z.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
iron_core.segment[:].name (alpha) | STR_0D | Name of the segment | ||
iron_core.segment[:].permeability_relative (alpha) | [iron_core.segment[:].b_field] | FLT_1D (uncertain) | - | Relative permeability of the iron segment |
iron_core.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
magnetics (alpha) | Magnetic diagnostics for equilibrium identification and plasma shape control. | |||
magnetics.bpol_probe (alpha) | [1...N] | STRUCT_ARRAY | Poloidal field probes | |
magnetics.bpol_probe[:].area (alpha) | FLT_0D (uncertain) | m^2 | Area of each turn of the coil | |
magnetics.bpol_probe[:].field (alpha) | STRUCTURE | Measured magnetic field | ||
magnetics.bpol_probe[:].field.data (alpha) | [magnetics.bpol_probe[:].field.time] | FLT_1D (uncertain) | T | Measured magnetic field |
magnetics.bpol_probe[:].field.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
magnetics.bpol_probe[:].identifier (alpha) | STR_0D | ID of the probe | ||
magnetics.bpol_probe[:].length (alpha) | FLT_0D (uncertain) | m | Length of the coil | |
magnetics.bpol_probe[:].name (alpha) | STR_0D | Name of the probe | ||
magnetics.bpol_probe[:].poloidal_angle (alpha) | FLT_0D (uncertain) | rad | Poloidal angle of the coil orientation | |
magnetics.bpol_probe[:].position (alpha) | STRUCTURE | R, Z, Phi position of the coil centre | ||
magnetics.bpol_probe[:].position.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
magnetics.bpol_probe[:].position.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
magnetics.bpol_probe[:].position.z (alpha) | FLT_0D (uncertain) | m | Height | |
magnetics.bpol_probe[:].toroidal_angle (alpha) | FLT_0D (uncertain) | rad | Toroidal angle of coil orientation (0 if fully in the poloidal plane) | |
magnetics.bpol_probe[:].turns (alpha) | INT_0D | Turns in the coil, including sign | ||
magnetics.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
magnetics.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
magnetics.code.name (alpha) | STR_0D | Name of software generating IDS | ||
magnetics.code.output_flag (alpha) | [magnetics.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
magnetics.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
magnetics.code.repository (alpha) | STR_0D | URL of software repository | ||
magnetics.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
magnetics.flux_loop (alpha) | [1...N] | STRUCT_ARRAY | Flux loops; partial flux loops can be described | |
magnetics.flux_loop[:].flux (alpha) | STRUCTURE | Measured flux | ||
magnetics.flux_loop[:].flux.data (alpha) | [magnetics.flux_loop[:].flux.time] | FLT_1D (uncertain) | Wb | Measured flux |
magnetics.flux_loop[:].flux.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
magnetics.flux_loop[:].identifier (alpha) | STR_0D | ID of the flux loop | ||
magnetics.flux_loop[:].name (alpha) | STR_0D | Name of the flux loop | ||
magnetics.flux_loop[:].position (alpha) | [1...N] | STRUCT_ARRAY | List of (R,Z,phi) points defining the position of the loop (see data structure documentation FLUXLOOPposition.pdf) | |
magnetics.flux_loop[:].position[:].phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
magnetics.flux_loop[:].position[:].r (alpha) | FLT_0D (uncertain) | m | Major radius | |
magnetics.flux_loop[:].position[:].z (alpha) | FLT_0D (uncertain) | m | Height | |
magnetics.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
magnetics.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
magnetics.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
magnetics.ids_properties.occurrence | INT_0D | |||
magnetics.method (alpha) | [1...N] | STRUCT_ARRAY | A method generating processed quantities derived from the magnetic measurements | |
magnetics.method[:].diamagnetic_flux (alpha) | STRUCTURE | Diamagnetic flux | ||
magnetics.method[:].diamagnetic_flux.data (alpha) | [magnetics.method[:].diamagnetic_flux.time] | FLT_1D (uncertain) | Wb | Diamagnetic flux |
magnetics.method[:].diamagnetic_flux.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
magnetics.method[:].ip (alpha) | STRUCTURE | Plasma current. Positive sign means anti-clockwise when viewed from above. | ||
magnetics.method[:].ip.data (alpha) | [magnetics.method[:].ip.time] | FLT_1D (uncertain) | A | Plasma current. Positive sign means anti-clockwise when viewed from above. |
magnetics.method[:].ip.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
magnetics.method[:].name (alpha) | STR_0D | Name of the data processing method | ||
magnetics.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
mhd_linear (alpha) | Magnetohydronamic linear stability | |||
mhd_linear.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
mhd_linear.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
mhd_linear.code.name (alpha) | STR_0D | Name of software generating IDS | ||
mhd_linear.code.output_flag (alpha) | [mhd_linear.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
mhd_linear.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
mhd_linear.code.repository (alpha) | STR_0D | URL of software repository | ||
mhd_linear.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
mhd_linear.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
mhd_linear.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
mhd_linear.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
mhd_linear.ids_properties.occurrence | INT_0D | |||
mhd_linear.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
mhd_linear.time_slice (alpha) | [mhd_linear.time_slice[:].time] | STRUCT_ARRAY | Core plasma radial profiles for various time slices | |
mhd_linear.time_slice[:].time (alpha) | FLT_0D | s | Time | |
mhd_linear.time_slice[:].toroidal_mode (alpha) | [1...N] | STRUCT_ARRAY | Vector of toroidal modes | |
mhd_linear.time_slice[:].toroidal_mode[:].frequency (alpha) | FLT_0D (uncertain) | Hz | Frequency of the mode | |
mhd_linear.time_slice[:].toroidal_mode[:].growthrate (alpha) | FLT_0D (uncertain) | Hz | Linear growthrate of the mode | |
mhd_linear.time_slice[:].toroidal_mode[:].n_tor (alpha) | INT_0D | Toroidal mode number of the MHD mode | ||
mhd_linear.time_slice[:].toroidal_mode[:].plasma (alpha) | STRUCTURE | MHD modes in the confined plasma | ||
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed (alpha) | STRUCTURE | T.m | Pertubed vector potential for given toroidal mode number | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate1 (alpha) | STRUCTURE | T.m | First coordinate (radial) | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate1.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T.m | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate1.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T.m | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate2 (alpha) | STRUCTURE | T.m | Second coordinate (poloidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate2.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T.m | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate2.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T.m | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate3 (alpha) | STRUCTURE | T.m | Third coordinate (toroidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate3.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T.m | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.a_field_perturbed.coordinate3.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T.m | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed (alpha) | STRUCTURE | T | Pertubed magnetic field for given toroidal mode number | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate1 (alpha) | STRUCTURE | T | First coordinate (radial) | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate1.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate1.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate2 (alpha) | STRUCTURE | T | Second coordinate (poloidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate2.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate2.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate3 (alpha) | STRUCTURE | T | Third coordinate (toroidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate3.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.b_field_perturbed.coordinate3.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | T | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_parallel (alpha) | STRUCTURE | m | Parallel displacement of the modes | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_parallel.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_parallel.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_perpendicular (alpha) | STRUCTURE | m | Perpendicular displacement of the modes | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_perpendicular.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.displacement_perpendicular.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid (alpha) | STRUCTURE | Definition of the 2D grid | ||
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1 (alpha) | [1...N] | FLT_1D (uncertain) | mixed | First dimension values |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim2 (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Second dimension values |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.volume_element (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m^3 | Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i) dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)] |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid_type (alpha) | STRUCTURE | Selection of one of a set of grid types | ||
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid_type.description (alpha) | STR_0D | Verbose description | ||
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid_type.name (alpha) | STR_0D | Short string identifier | ||
mhd_linear.time_slice[:].toroidal_mode[:].plasma.mass_density_perturbed (alpha) | STRUCTURE | kg.m^-3 | Perturbed mass density for given toroidal mode number | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.mass_density_perturbed.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | kg.m^-3 | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.mass_density_perturbed.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | kg.m^-3 | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.pressure_perturbed (alpha) | STRUCTURE | Pa | Perturbed pressure for given toroidal mode number | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.pressure_perturbed.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | Pa | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.pressure_perturbed.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | Pa | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.tau_alfven (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1] | FLT_1D (uncertain) | s | Alven time=R/vA=R0 sqrt(mi ni(rho))/B0 |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.tau_resistive (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1] | FLT_1D (uncertain) | s | Resistive time = mu_0 rho*rho/1.22/eta_neo |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.temperature_perturbed (alpha) | STRUCTURE | eV | Perturbed temperature for given toroidal mode number | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.temperature_perturbed.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | eV | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.temperature_perturbed.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | eV | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed (alpha) | STRUCTURE | m/s | Pertubed velocity for given toroidal mode number | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate1 (alpha) | STRUCTURE | m/s | First coordinate (radial) | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate1.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m/s | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate1.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m/s | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate2 (alpha) | STRUCTURE | m/s | Second coordinate (poloidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate2.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m/s | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate2.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m/s | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate3 (alpha) | STRUCTURE | m/s | Third coordinate (toroidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate3.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m/s | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].plasma.velocity_perturbed.coordinate3.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].plasma.grid.dim1, | FLT_2D (uncertain) | m/s | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum (alpha) | STRUCTURE | MHD modes in the vaccum | ||
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed (alpha) | STRUCTURE | T.m | Pertubed vector potential for given toroidal mode number | |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed.coordinate1 (alpha) | STRUCTURE | T.m | First coordinate (radial) | |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed.coordinate1.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T.m | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed.coordinate1.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T.m | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed.coordinate2 (alpha) | STRUCTURE | T.m | Second coordinate (poloidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed.coordinate2.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T.m | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed.coordinate2.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T.m | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed.coordinate3 (alpha) | STRUCTURE | T.m | Third coordinate (toroidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed.coordinate3.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T.m | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.a_field_perturbed.coordinate3.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T.m | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed (alpha) | STRUCTURE | T | Pertubed magnetic field for given toroidal mode number | |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed.coordinate1 (alpha) | STRUCTURE | T | First coordinate (radial) | |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed.coordinate1.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed.coordinate1.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed.coordinate2 (alpha) | STRUCTURE | T | Second coordinate (poloidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed.coordinate2.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed.coordinate2.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed.coordinate3 (alpha) | STRUCTURE | T | Third coordinate (toroidal) | |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed.coordinate3.imaginary (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T | Imaginary part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.b_field_perturbed.coordinate3.real (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | T | Real part |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid (alpha) | STRUCTURE | Definition of the 2D grid | ||
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1 (alpha) | [1...N] | FLT_1D (uncertain) | mixed | First dimension values |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim2 (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Second dimension values |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.volume_element (alpha) | [mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid.dim1, | FLT_2D (uncertain) | m^3 | Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i) dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)] |
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid_type (alpha) | STRUCTURE | Selection of one of a set of grid types | ||
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid_type.description (alpha) | STR_0D | Verbose description | ||
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
mhd_linear.time_slice[:].toroidal_mode[:].vaccuum.grid_type.name (alpha) | STR_0D | Short string identifier | ||
mhd_linear.vacuum_toroidal_field (alpha) | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities) | ||
mhd_linear.vacuum_toroidal_field.b0 (alpha) | [mhd_linear.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
mhd_linear.vacuum_toroidal_field.r0 (alpha) | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
nbi (alpha) | Neutral Beam Injection systems and description of the fast neutrals that arrive into the torus | |||
nbi.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
nbi.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
nbi.code.name (alpha) | STR_0D | Name of software generating IDS | ||
nbi.code.output_flag (alpha) | [nbi.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
nbi.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
nbi.code.repository (alpha) | STR_0D | URL of software repository | ||
nbi.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
nbi.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
nbi.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
nbi.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
nbi.ids_properties.occurrence | INT_0D | |||
nbi.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
nbi.unit (alpha) | [1...N] | STRUCT_ARRAY | The NBI system is described as a set of units of which the power can be controlled individually. | |
nbi.unit[:].beam_current_fraction (alpha) | STRUCTURE | Fractions of beam current distributed among the different energies, the first index corresponds to the fast neutrals energy (1:full, 2: half, 3: one third) | ||
nbi.unit[:].beam_current_fraction.data (alpha) | [1...3, | FLT_2D (uncertain) | - | Fractions of beam current distributed among the different energies, the first index corresponds to the fast neutrals energy (1:full, 2: half, 3: one third) |
nbi.unit[:].beam_current_fraction.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
nbi.unit[:].beam_power_fraction (alpha) | STRUCTURE | Fractions of beam power distributed among the different energies, the first index corresponds to the fast neutrals energy (1:full, 2: half, 3: one third) | ||
nbi.unit[:].beam_power_fraction.data (alpha) | [1...3, | FLT_2D (uncertain) | - | Fractions of beam power distributed among the different energies, the first index corresponds to the fast neutrals energy (1:full, 2: half, 3: one third) |
nbi.unit[:].beam_power_fraction.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
nbi.unit[:].beamlets_group (alpha) | [1...N] | STRUCT_ARRAY | Group of beamlets with common vertical and horizontal focal point. If there are no common focal points, then select small groups of beamlets such that a focal point description of the beamlets group provides a fair description | |
nbi.unit[:].beamlets_group[:].angle (alpha) | FLT_0D (uncertain) | rad | Angle of inclination between a beamlet at the centre of the injection unit surface and the horiontal plane | |
nbi.unit[:].beamlets_group[:].beamlets (alpha) | STRUCTURE | Detailed information on beamlets | ||
nbi.unit[:].beamlets_group[:].beamlets.angles (alpha) | [nbi.unit[:].beamlets_group[:].beamlets.positions.R] | FLT_1D (uncertain) | rad | Angle of inclination between a line at the centre of a beamlet and the horiontal plane, for each beamlet |
nbi.unit[:].beamlets_group[:].beamlets.positions (alpha) | STRUCTURE | Position of each beamlet | ||
nbi.unit[:].beamlets_group[:].beamlets.positions.phi (alpha) | [nbi.unit[:].beamlets_group[:].beamlets.positions.r] | FLT_1D (uncertain) | rad | Toroidal angle |
nbi.unit[:].beamlets_group[:].beamlets.positions.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
nbi.unit[:].beamlets_group[:].beamlets.positions.z (alpha) | [nbi.unit[:].beamlets_group[:].beamlets.positions.r] | FLT_1D (uncertain) | m | Height |
nbi.unit[:].beamlets_group[:].beamlets.power_fractions (alpha) | [nbi.unit[:].beamlets_group[:].beamlets.positions.R] | FLT_1D (uncertain) | rad | Fraction of power of a unit injected by each beamlet |
nbi.unit[:].beamlets_group[:].beamlets.tangency_radii (alpha) | [nbi.unit[:].beamlets_group[:].beamlets.positions.R] | FLT_1D (uncertain) | m | Tangency radius (major radius where the central line of a beamlet is tangent to a circle around the torus), for each beamlet |
nbi.unit[:].beamlets_group[:].direction (alpha) | INT_0D | Direction of the beam seen from above the torus: -1 = clockwise; 1 = counter clockwise | ||
nbi.unit[:].beamlets_group[:].divergence_component (alpha) | [1...N] | STRUCT_ARRAY | Detailed information on beamlet divergence. Divergence is described as a superposition of Gaussian components with amplitide "particles_fraction" and vertical/horizontal divergence. Note that for positive ion NBI the divergence is well described by a single Gaussian | |
nbi.unit[:].beamlets_group[:].divergence_component[:].horizontal (alpha) | FLT_0D (uncertain) | rad | The horiztonal beamlet divergence of the component. Here the divergence is defined for Gaussian beams as the angel where the beam density is reduced by a factor 1/e compared to the maximum density. For non-Gaussian beams the divergence is sqrt(2)*mean((x-mean(x))**2), where x is the angle and the mean should be performed over the beam density, P(x): mean(y)=int(y*P(x)*dx). | |
nbi.unit[:].beamlets_group[:].divergence_component[:].particles_fraction (alpha) | FLT_0D (uncertain) | - | Fraction of injected particles in the component | |
nbi.unit[:].beamlets_group[:].divergence_component[:].vertical (alpha) | FLT_0D (uncertain) | rad | The vertical beamlet divergence of the component. Here the divergence is defined for Gaussian beams as the angel where the beam density is reduced by a factor 1/e compared to the maximum density. For non-Gaussian beams the divergence is sqrt(2)*mean((x-mean(x))**2), where x is the angle and the mean should be performed over the beam density, P(x): mean(y)=int(y*P(x)*dx). | |
nbi.unit[:].beamlets_group[:].focus (alpha) | STRUCTURE | Describes how the beamlet group is focused | ||
nbi.unit[:].beamlets_group[:].focus.focal_length_horizontal (alpha) | FLT_0D (uncertain) | m | Horizontal focal length along the beam line, i.e. the point along the centre of the beamlet-group where the beamlet-group has its minimum horizontal width | |
nbi.unit[:].beamlets_group[:].focus.focal_length_vertical (alpha) | FLT_0D (uncertain) | m | Vertical focal length along the beam line, i.e. the point along the centre of the beamlet-group where the beamlet-group has its minimum vertical width | |
nbi.unit[:].beamlets_group[:].focus.width_min_horizontal (alpha) | FLT_0D (uncertain) | m | The horizontal width of the beamlets group at the at the horizontal focal point | |
nbi.unit[:].beamlets_group[:].focus.width_min_vertical (alpha) | FLT_0D (uncertain) | m | The vertical width of the beamlets group at the at the vertical focal point | |
nbi.unit[:].beamlets_group[:].position (alpha) | STRUCTURE | R, Z, Phi position of the beamlet group centre | ||
nbi.unit[:].beamlets_group[:].position.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
nbi.unit[:].beamlets_group[:].position.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
nbi.unit[:].beamlets_group[:].position.z (alpha) | FLT_0D (uncertain) | m | Height | |
nbi.unit[:].beamlets_group[:].tangency_radius (alpha) | FLT_0D (uncertain) | m | Tangency radius (major radius where the central line of a NBI unit is tangent to a circle around the torus) | |
nbi.unit[:].beamlets_group[:].width_horizontal (alpha) | FLT_0D (uncertain) | m | Horizontal width of the beam group at the injection unit surface (or grounded grid) | |
nbi.unit[:].beamlets_group[:].width_vertical (alpha) | FLT_0D (uncertain) | m | Vertical width of the beam group at the injection unit surface (or grounded grid) | |
nbi.unit[:].energy (alpha) | STRUCTURE | Full energy of the injected species (acceleration of a single atom) | ||
nbi.unit[:].energy.data (alpha) | [nbi.unit[:].energy.time] | FLT_1D (uncertain) | eV | Full energy of the injected species (acceleration of a single atom) |
nbi.unit[:].energy.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
nbi.unit[:].identifier (alpha) | STR_0D | ID of the NBI unit | ||
nbi.unit[:].name (alpha) | STR_0D | Name of the NBI unit | ||
nbi.unit[:].power (alpha) | STRUCTURE | Power | ||
nbi.unit[:].power.data (alpha) | [nbi.unit[:].power.time] | FLT_1D (uncertain) | W | Power |
nbi.unit[:].power.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
nbi.unit[:].species (alpha) | STRUCTURE | Atomic Mass Unit | Injected species | |
nbi.unit[:].species.a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
nbi.unit[:].species.label (alpha) | STR_0D | String identifying the species (e.g. H, D, T, ...) | ||
nbi.unit[:].species.z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
neutron_diagnostic (alpha) | Neutron diagnostic such as DNFM, NFM or MFC | |||
neutron_diagnostic.characteristics (alpha) | STRUCTURE | Description of Diagnostic's module detection characteristics for differen plasma modes based on Design Description | ||
neutron_diagnostic.characteristics.dead_time (alpha) | FLT_0D (uncertain) | s | Dead time of detectors | |
neutron_diagnostic.characteristics.pulse_length (alpha) | FLT_0D (uncertain) | s | Lower counting limit of recent Measuring Mode and plasma reaction | |
neutron_diagnostic.characteristics.reaction (alpha) | [neutron_diagnostic.characteristics.reaction[:].index] | STRUCT_ARRAY | Plasma reaction (1 -'DT'; 2 - 'DD') | |
neutron_diagnostic.characteristics.reaction[:].error (alpha) | FLT_0D (uncertain) | - | Diagnostic's relative uncertainty for recent plasma reaction | |
neutron_diagnostic.characteristics.reaction[:].index (alpha) | INT_0D | Index of plasma reaction type | ||
neutron_diagnostic.characteristics.reaction[:].mode (alpha) | [neutron_diagnostic.characteristics.reaction[:].mode[:].index] | STRUCT_ARRAY | Characteristics of counting linear limits in recent Measuring modes for recent Plasma reaction type | |
neutron_diagnostic.characteristics.reaction[:].mode[:].count_limit_max (alpha) | FLT_0D (uncertain) | cps | Maximum count limit of recent Measuring Mode and plasma reaction | |
neutron_diagnostic.characteristics.reaction[:].mode[:].count_limit_min (alpha) | FLT_0D (uncertain) | cps | Minimum count limit of recent Measuring Mode and plasma reaction | |
neutron_diagnostic.characteristics.reaction[:].mode[:].index (alpha) | INT_0D | Index of Measuring Mode | ||
neutron_diagnostic.characteristics.reaction[:].mode[:].name (alpha) | STR_0D | Name of Measuring Mode | ||
neutron_diagnostic.characteristics.reaction[:].probability_overlap (alpha) | FLT_0D (uncertain) | - | Pulse probability overlap for recent plasma reaction | |
neutron_diagnostic.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
neutron_diagnostic.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
neutron_diagnostic.code.name (alpha) | STR_0D | Name of software generating IDS | ||
neutron_diagnostic.code.output_flag (alpha) | [neutron_diagnostic.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
neutron_diagnostic.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
neutron_diagnostic.code.repository (alpha) | STR_0D | URL of software repository | ||
neutron_diagnostic.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
neutron_diagnostic.detectors (alpha) | [1...N] | STRUCT_ARRAY | Description of Detectors properties and Data in Neutron Diagnostic Module | |
neutron_diagnostic.detectors[:].index (alpha) | INT_0D | Number of Detector. TO BE REMOVED: the detector index is provided by the index of the detector array above. | ||
neutron_diagnostic.detectors[:].mode (alpha) | [neutron_diagnostic.detectors[:].mode[:].index] | STRUCT_ARRAY | Measuring Mode Properties and Data | |
neutron_diagnostic.detectors[:].mode[:].counting (alpha) | STRUCTURE | Counting in Measuring Mode in Dynamic | ||
neutron_diagnostic.detectors[:].mode[:].counting.data (alpha) | [neutron_diagnostic.time] | FLT_1D (uncertain) | cps | Counting in Measuring Mode in Dynamic |
neutron_diagnostic.detectors[:].mode[:].counting.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
neutron_diagnostic.detectors[:].mode[:].index (alpha) | INT_0D | Index of Measuring Mode. TO BE REMOVED: the mode index is provided by the index of the mode array above. | ||
neutron_diagnostic.detectors[:].mode[:].name (alpha) | STR_0D | Name of Measuring Mode | ||
neutron_diagnostic.detectors[:].name (alpha) | STR_0D | Name of Detector | ||
neutron_diagnostic.detectors[:].position (alpha) | STRUCTURE | Detector Position Data | ||
neutron_diagnostic.detectors[:].position.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
neutron_diagnostic.detectors[:].position.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
neutron_diagnostic.detectors[:].position.z (alpha) | FLT_0D (uncertain) | m | Height | |
neutron_diagnostic.detectors[:].radiation (alpha) | [neutron_diagnostic.detectors[:].radiation[:].index] | STRUCT_ARRAY | Radiation type on detector's converter (1 - 'neutrons'; 2 - 'gamma-rays') | |
neutron_diagnostic.detectors[:].radiation[:].converter_name (alpha) | STR_0D | Name of detector's converter for resent particle | ||
neutron_diagnostic.detectors[:].radiation[:].converter_nuclear_density (alpha) | FLT_0D (uncertain) | m^-3 | Nuclear density of detector's converter for resent particle | |
neutron_diagnostic.detectors[:].radiation[:].converter_temperature (alpha) | [neutron_diagnostic.time] | FLT_1D (uncertain) | K | Temperature of detector's converter |
neutron_diagnostic.detectors[:].radiation[:].converter_volume (alpha) | FLT_0D (uncertain) | m^3 | Volume of detector's converter for resent particle | |
neutron_diagnostic.detectors[:].radiation[:].index (alpha) | INT_0D | Index of radiation type | ||
neutron_diagnostic.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
neutron_diagnostic.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
neutron_diagnostic.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
neutron_diagnostic.ids_properties.occurrence | INT_0D | |||
neutron_diagnostic.synthetic_signals (alpha) | STRUCTURE | Output Data from Neutron Diagnostic's Module | ||
neutron_diagnostic.synthetic_signals.fusion_power (alpha) | [neutron_diagnostic.time] | FLT_1D (uncertain) | W | Fusion Power |
neutron_diagnostic.synthetic_signals.total_neutron_flux (alpha) | [neutron_diagnostic.time] | FLT_1D (uncertain) | s^-1 | Total Neutron Flux in Dynamic |
neutron_diagnostic.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
neutron_diagnostic.unit_source (alpha) | [1...N] | STRUCT_ARRAY | Unit ring sources description | |
neutron_diagnostic.unit_source[:].position (alpha) | STRUCTURE | Position of ring unit sources inside ITER vacuum vessel | ||
neutron_diagnostic.unit_source[:].position.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
neutron_diagnostic.unit_source[:].position.z (alpha) | FLT_0D (uncertain) | m | Height | |
neutron_diagnostic.unit_source[:].radiation (alpha) | [neutron_diagnostic.unit_source[:].radiation[:].index] | STRUCT_ARRAY | Radiation type on detector's converter (1 - 'neutrons'; 2 - 'gamma-rays') | |
neutron_diagnostic.unit_source[:].radiation[:].index (alpha) | INT_0D | Index of radiation type. TO BE REMOVED, since it is given by the index of the radiation array above. | ||
neutron_diagnostic.unit_source[:].radiation[:].reaction (alpha) | [neutron_diagnostic.unit_source[:].radiation[:].reaction[:].index] | STRUCT_ARRAY | Plasma reaction (1 - 'DT'; 2 - 'DD') | |
neutron_diagnostic.unit_source[:].radiation[:].reaction[:].d2flux_drdz (alpha) | [1...N, | FLT_2D (uncertain) | m^-4 | Second deriviation of Radiation flux from Unit Ring Source in recent detector's converter for "spline" reconstruction(1 - Number of Detector, 2 - Energy of particles) |
neutron_diagnostic.unit_source[:].radiation[:].reaction[:].energy (alpha) | [1...N] | FLT_1D (uncertain) | eV | Energy boundaries for Detector Radiator Flux |
neutron_diagnostic.unit_source[:].radiation[:].reaction[:].flux (alpha) | [1...N, | FLT_2D (uncertain) | m^-2 | Radiation flux from Unit Ring Source in recent detector's converter (1 - Number of Detector, 2 - Energy of particles) |
neutron_diagnostic.unit_source[:].radiation[:].reaction[:].index (alpha) | INT_0D | Index of plasma reaction type. To be removed, since it is given by the index of the reaction array above. | ||
neutron_diagnostic.unit_source[:].radiation[:].reaction[:].reaction_rate (alpha) | [1...N, | FLT_2D (uncertain) | m^-3 | Reaction Rate on converter's material from Unit Ring Source in recent detector's converter (1 - Number of Detector, 2 - Energy of particles) |
neutron_diagnostic.unit_source[:].radiation[:].reaction[:].sensitivity (alpha) | [1...N, | FLT_2D (uncertain) | cps.m^2.s | Sensitivity of converter's material in recent detector's converter (1 - Number of Detector, 2 - Energy of particles) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
ntms (alpha) | Description of neoclassical tearing modes | |||
ntms.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
ntms.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
ntms.code.name (alpha) | STR_0D | Name of software generating IDS | ||
ntms.code.output_flag (alpha) | [ntms.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
ntms.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
ntms.code.repository (alpha) | STR_0D | URL of software repository | ||
ntms.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
ntms.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
ntms.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
ntms.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
ntms.ids_properties.occurrence | INT_0D | |||
ntms.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
ntms.time_slice (alpha) | [ntms.time_slice[:].time] | STRUCT_ARRAY | Description of neoclassical tearing modes for various time slices | |
ntms.time_slice[:].mode (alpha) | [1...N] | STRUCT_ARRAY | List of the various NTM modes appearing during the simulation. If a mode appears several times, use several indices in this array of structure with the same m,n values. | |
ntms.time_slice[:].mode[:].calculation_method (alpha) | STR_0D | Description of how the mode evolution is calculated | ||
ntms.time_slice[:].mode[:].delta_diff (alpha) | [1...3] | FLT_1D (uncertain) | m^2.s^-1 | Extra diffusion coefficient for the transport equations of Te, ne, Ti |
ntms.time_slice[:].mode[:].deltaw (alpha) | [1...N] | STRUCT_ARRAY | deltaw contributions to the Rutherford equation | |
ntms.time_slice[:].mode[:].deltaw[:].name (alpha) | STR_0D | Name of the contribution | ||
ntms.time_slice[:].mode[:].deltaw[:].value (alpha) | FLT_0D (uncertain) | m^-1 | Value of the contribution | |
ntms.time_slice[:].mode[:].detailed_evolution (alpha) | STRUCTURE | Detailed NTM evolution on a finer timebase than the time_slice array of structure | ||
ntms.time_slice[:].mode[:].detailed_evolution.calculation_method (alpha) | STR_0D | Description of how the mode evolution is calculated | ||
ntms.time_slice[:].mode[:].detailed_evolution.delta_diff (alpha) | [1...3, | FLT_2D (uncertain) | m^2.s^-1 | Extra diffusion coefficient for the transport equations of Te, ne, Ti |
ntms.time_slice[:].mode[:].detailed_evolution.deltaw (alpha) | [1...N] | STRUCT_ARRAY | deltaw contributions to the Rutherford equation | |
ntms.time_slice[:].mode[:].detailed_evolution.deltaw[:].name (alpha) | STR_0D | Name of the contribution | ||
ntms.time_slice[:].mode[:].detailed_evolution.deltaw[:].value (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | m^-1 | Value of the contribution |
ntms.time_slice[:].mode[:].detailed_evolution.dfrequency_dt (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | s^-2 | Time derivative of the frequency of the mode |
ntms.time_slice[:].mode[:].detailed_evolution.dphase_dt (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | rad/s | Time derivative of the phase of the mode |
ntms.time_slice[:].mode[:].detailed_evolution.dwidth_dt (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | m/s | Time derivative of the full width of the mode |
ntms.time_slice[:].mode[:].detailed_evolution.frequency (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | Hz | Frequency of the mode |
ntms.time_slice[:].mode[:].detailed_evolution.m_pol (alpha) | INT_0D | Poloidal mode number | ||
ntms.time_slice[:].mode[:].detailed_evolution.n_tor (alpha) | INT_0D | Toroidal mode number | ||
ntms.time_slice[:].mode[:].detailed_evolution.phase (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | rad | Phase of the mode |
ntms.time_slice[:].mode[:].detailed_evolution.rho_tor (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | m | Flux coordinate on which the mode is centred |
ntms.time_slice[:].mode[:].detailed_evolution.rho_tor_norm (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | - | Normalised flux coordinate on which the mode is centred |
ntms.time_slice[:].mode[:].detailed_evolution.time_detailed (alpha) | [1...N] | FLT_1D (uncertain) | s | Time array used to describe the detailed evolution of the NTM |
ntms.time_slice[:].mode[:].detailed_evolution.torque (alpha) | [1...N] | STRUCT_ARRAY | torque contributions to the Rutherford equation | |
ntms.time_slice[:].mode[:].detailed_evolution.torque[:].name (alpha) | STR_0D | Name of the contribution | ||
ntms.time_slice[:].mode[:].detailed_evolution.torque[:].value (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | kg.m^2.s^-2 | Value of the contribution |
ntms.time_slice[:].mode[:].detailed_evolution.width (alpha) | [ntms.time_slice[:].mode[:].detailed_evolution.time_detailed] | FLT_1D (uncertain) | m | Full width of the mode |
ntms.time_slice[:].mode[:].dfrequency_dt (alpha) | FLT_0D (uncertain) | s^-2 | Time derivative of the frequency of the mode | |
ntms.time_slice[:].mode[:].dphase_dt (alpha) | FLT_0D (uncertain) | rad/s | Time derivative of the phase of the mode | |
ntms.time_slice[:].mode[:].dwidth_dt (alpha) | FLT_0D (uncertain) | m/s | Time derivative of the full width of the mode | |
ntms.time_slice[:].mode[:].frequency (alpha) | FLT_0D (uncertain) | Hz | Frequency of the mode | |
ntms.time_slice[:].mode[:].m_pol (alpha) | INT_0D | Poloidal mode number | ||
ntms.time_slice[:].mode[:].n_tor (alpha) | INT_0D | Toroidal mode number | ||
ntms.time_slice[:].mode[:].onset (alpha) | STRUCTURE | NTM onset characteristics | ||
ntms.time_slice[:].mode[:].onset.cause (alpha) | STR_0D | Cause of the mode onset | ||
ntms.time_slice[:].mode[:].onset.m_pol (alpha) | INT_0D | Poloidal mode number | ||
ntms.time_slice[:].mode[:].onset.n_tor (alpha) | INT_0D | Toroidal mode number | ||
ntms.time_slice[:].mode[:].onset.phase (alpha) | FLT_0D (uncertain) | rad | Phase of the mode at onset | |
ntms.time_slice[:].mode[:].onset.time_offset (alpha) | FLT_0D (uncertain) | s | Offset time (when a mode disappears). If the mode reappears later in the simulation, use another index of the mode array of structure | |
ntms.time_slice[:].mode[:].onset.time_onset (alpha) | FLT_0D (uncertain) | s | Onset time | |
ntms.time_slice[:].mode[:].onset.width (alpha) | FLT_0D (uncertain) | m | Seed island full width at onset time | |
ntms.time_slice[:].mode[:].phase (alpha) | FLT_0D (uncertain) | rad | Phase of the mode | |
ntms.time_slice[:].mode[:].rho_tor (alpha) | FLT_0D (uncertain) | m | Flux coordinate on which the mode is centred | |
ntms.time_slice[:].mode[:].rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Normalised flux coordinate on which the mode is centred | |
ntms.time_slice[:].mode[:].torque (alpha) | [1...N] | STRUCT_ARRAY | torque contributions to the Rutherford equation | |
ntms.time_slice[:].mode[:].torque[:].name (alpha) | STR_0D | Name of the contribution | ||
ntms.time_slice[:].mode[:].torque[:].value (alpha) | FLT_0D (uncertain) | kg.m^2.s^-2 | Value of the contribution | |
ntms.time_slice[:].mode[:].width (alpha) | FLT_0D (uncertain) | m | Full width of the mode | |
ntms.time_slice[:].time (alpha) | FLT_0D | s | Time | |
ntms.vacuum_toroidal_field (alpha) | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition) | ||
ntms.vacuum_toroidal_field.b0 (alpha) | [ntms.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
ntms.vacuum_toroidal_field.r0 (alpha) | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
pellets (alpha) | Description of pellets launched into the plasma | |||
pellets.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
pellets.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
pellets.code.name (alpha) | STR_0D | Name of software generating IDS | ||
pellets.code.output_flag (alpha) | [pellets.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
pellets.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
pellets.code.repository (alpha) | STR_0D | URL of software repository | ||
pellets.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
pellets.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
pellets.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
pellets.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
pellets.ids_properties.occurrence | INT_0D | |||
pellets.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pellets.time_slice (alpha) | [pellets.time_slice[:].time] | STRUCT_ARRAY | Description of the pellets launched at various time slices. The time of this structure corresponds to the full ablation of the pellet inside the plasma. | |
pellets.time_slice[:].pellet (alpha) | [1...N] | STRUCT_ARRAY | Set of pellets ablated in the plasma at a given time | |
pellets.time_slice[:].pellet[:].path_geometry (alpha) | STRUCTURE | Geometry of the pellet path in the vaccuum chamber | ||
pellets.time_slice[:].pellet[:].path_geometry.first_point (alpha) | STRUCTURE | Position of the first point | ||
pellets.time_slice[:].pellet[:].path_geometry.first_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
pellets.time_slice[:].pellet[:].path_geometry.first_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
pellets.time_slice[:].pellet[:].path_geometry.first_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
pellets.time_slice[:].pellet[:].path_geometry.second_point (alpha) | STRUCTURE | Position of the second point | ||
pellets.time_slice[:].pellet[:].path_geometry.second_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
pellets.time_slice[:].pellet[:].path_geometry.second_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
pellets.time_slice[:].pellet[:].path_geometry.second_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
pellets.time_slice[:].pellet[:].path_profiles (alpha) | STRUCTURE | 1-D profiles of plasma and pellet along the pellet path | ||
pellets.time_slice[:].pellet[:].path_profiles.ablated_particles (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.distance] | FLT_1D (uncertain) | - | Number of ablated particles (electrons) along the pellet path |
pellets.time_slice[:].pellet[:].path_profiles.ablation_rate (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.distance] | FLT_1D (uncertain) | s^-1 | Ablation rate (electrons) along the pellet path |
pellets.time_slice[:].pellet[:].path_profiles.distance (alpha) | [1...N] | FLT_1D (uncertain) | m | Distance along the pellet path, with the origin taken at path_geometry/first_point. Used as the main coordinate for the path_profiles structure |
pellets.time_slice[:].pellet[:].path_profiles.n_e (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.distance] | FLT_1D (uncertain) | m^-3 | Electron density along the pellet path |
pellets.time_slice[:].pellet[:].path_profiles.position (alpha) | STRUCTURE | Position along the pellet path | ||
pellets.time_slice[:].pellet[:].path_profiles.position.phi (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.position.r] | FLT_1D (uncertain) | rad | Toroidal angle |
pellets.time_slice[:].pellet[:].path_profiles.position.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
pellets.time_slice[:].pellet[:].path_profiles.position.z (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.position.r] | FLT_1D (uncertain) | m | Height |
pellets.time_slice[:].pellet[:].path_profiles.psi (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.distance] | FLT_1D (uncertain) | Wb | Poloidal flux along the pellet path |
pellets.time_slice[:].pellet[:].path_profiles.rho_tor_norm (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.distance] | FLT_1D (uncertain) | - | Normalised toroidal coordinate along the pellet path |
pellets.time_slice[:].pellet[:].path_profiles.rho_tor_norm_drift (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.distance] | FLT_1D (uncertain) | - | Difference to due ExB drifts between the ablation and the final deposition locations, in terms of the normalised toroidal flux coordinate |
pellets.time_slice[:].pellet[:].path_profiles.t_e (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.distance] | FLT_1D (uncertain) | eV | Electron temperature along the pellet path |
pellets.time_slice[:].pellet[:].path_profiles.velocity (alpha) | [pellets.time_slice[:].pellet[:].path_profiles.distance] | FLT_1D (uncertain) | m.s^-1 | Pellet velocity along the pellet path |
pellets.time_slice[:].pellet[:].shape (alpha) | STRUCTURE | Initial shape of a pellet at launch | ||
pellets.time_slice[:].pellet[:].shape.size (alpha) | [1...N] | FLT_1D (uncertain) | m | Size of the pellet in the various dimensions, depending on the shape type. Spherical pellets: size(1) is the radius of the pellet. Cylindrical pellets: size(1) is the radius and size(2) is the height of the cylinder. Rectangular pellets: size(1) is the height, size(2) is the width and size(3) is the length |
pellets.time_slice[:].pellet[:].shape.type (alpha) | STRUCTURE | Identifier structure for the shape type: 1-spherical; 2-cylindrical; 3-rectangular | ||
pellets.time_slice[:].pellet[:].shape.type.description (alpha) | STR_0D | Verbose description | ||
pellets.time_slice[:].pellet[:].shape.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
pellets.time_slice[:].pellet[:].shape.type.name (alpha) | STR_0D | Short string identifier | ||
pellets.time_slice[:].pellet[:].species (alpha) | [1...N] | STRUCT_ARRAY | Set of species included in the pellet composition | |
pellets.time_slice[:].pellet[:].species[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
pellets.time_slice[:].pellet[:].species[:].density (alpha) | FLT_0D (uncertain) | - | Material density of the species in the pellet | |
pellets.time_slice[:].pellet[:].species[:].fraction (alpha) | FLT_0D (uncertain) | - | Fraction of the species atoms in the pellet | |
pellets.time_slice[:].pellet[:].species[:].label (alpha) | STR_0D | String identifying the species (e.g. H, D, T, ...) | ||
pellets.time_slice[:].pellet[:].species[:].sublimation_energy (alpha) | FLT_0D (uncertain) | eV | Sublimation energy per atom | |
pellets.time_slice[:].pellet[:].species[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
pellets.time_slice[:].pellet[:].velocity_initial (alpha) | FLT_0D (uncertain) | m.s^-1 | Initial velocity of the pellet as it enters the vaccum chamber | |
pellets.time_slice[:].time (alpha) | FLT_0D | s | Time |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
pf_active (alpha) | Description of the axisymmetric active poloidal field (PF) coils and supplies; includes the limits of these systems; includes the forces on them; does not include non-axisymmetric coil systems | |||
pf_active.circuit (alpha) | [1...N] | STRUCT_ARRAY | Circuits, connecting multiple PF coils to multiple supplies, defining the current and voltage relationships in the system | |
pf_active.circuit[:].connections (alpha) | [1...N, | INT_2D | Description of the supplies and coils connections (nodes) across the circuit. Nodes of the circuit are listed as the first dimension of the matrix. Supplies (listed first) and coils (listed second) SIDES are listed as the second dimension. Thus the second dimension has a size equal to 2*(N_supplies+N_coils). The (i,j) matrix elements are 1 if the j-th supply or coil side is connected to the i-th node, or 0 otherwise. | |
pf_active.circuit[:].current (alpha) | STRUCTURE | Current in the circuit | ||
pf_active.circuit[:].current.data (alpha) | [pf_active.circuit[:].current.time] | FLT_1D (uncertain) | V | Current in the circuit |
pf_active.circuit[:].current.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pf_active.circuit[:].identifier (alpha) | STR_0D | ID of the circuit | ||
pf_active.circuit[:].name (alpha) | STR_0D | Name of the circuit | ||
pf_active.circuit[:].type (alpha) | STR_0D | Type of the circuit | ||
pf_active.circuit[:].voltage (alpha) | STRUCTURE | Voltage on the circuit | ||
pf_active.circuit[:].voltage.data (alpha) | [pf_active.circuit[:].voltage.time] | FLT_1D (uncertain) | V | Voltage on the circuit |
pf_active.circuit[:].voltage.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pf_active.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
pf_active.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
pf_active.code.name (alpha) | STR_0D | Name of software generating IDS | ||
pf_active.code.output_flag (alpha) | [pf_active.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
pf_active.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
pf_active.code.repository (alpha) | STR_0D | URL of software repository | ||
pf_active.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
pf_active.coil (alpha) | [1...N] | STRUCT_ARRAY | Active PF coils | |
pf_active.coil[:].current (alpha) | STRUCTURE | Current in the coil | ||
pf_active.coil[:].current.data (alpha) | [pf_active.coil[:].current.time] | FLT_1D (uncertain) | A | Current in the coil |
pf_active.coil[:].current.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pf_active.coil[:].element (alpha) | [1...N] | STRUCT_ARRAY | Each PF coil is comprised of a number of cross-section elements described individually | |
pf_active.coil[:].element[:].area (alpha) | FLT_0D (uncertain) | m^2 | Cross-sectional areas of the element | |
pf_active.coil[:].element[:].geometry (alpha) | STRUCTURE | Cross-sectional shape of the element | ||
pf_active.coil[:].element[:].geometry.geometry_type (alpha) | INT_0D | Type used to describe the element shape (1:'outline', 2:'rectangle', 3:'oblique') | ||
pf_active.coil[:].element[:].geometry.oblique (alpha) | STRUCTURE | Trapezoidal description of the element | ||
pf_active.coil[:].element[:].geometry.oblique.alpha (alpha) | FLT_0D (uncertain) | m | Inclination of first angle TBD | |
pf_active.coil[:].element[:].geometry.oblique.beta (alpha) | FLT_0D (uncertain) | m | Inclination of second angle TBD | |
pf_active.coil[:].element[:].geometry.oblique.length (alpha) | FLT_0D (uncertain) | m | Length | |
pf_active.coil[:].element[:].geometry.oblique.r (alpha) | FLT_0D (uncertain) | m | Geometric centre R | |
pf_active.coil[:].element[:].geometry.oblique.thickness (alpha) | FLT_0D (uncertain) | m | Thickness | |
pf_active.coil[:].element[:].geometry.oblique.z (alpha) | FLT_0D (uncertain) | m | Geometric centre Z | |
pf_active.coil[:].element[:].geometry.outline (alpha) | STRUCTURE | Irregular outline of the element | ||
pf_active.coil[:].element[:].geometry.outline.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
pf_active.coil[:].element[:].geometry.outline.z (alpha) | [pf_active.coil[:].element[:].geometry.outline.r] | FLT_1D (uncertain) | m | Height |
pf_active.coil[:].element[:].geometry.rectangle (alpha) | STRUCTURE | Rectangular description of the element | ||
pf_active.coil[:].element[:].geometry.rectangle.height (alpha) | FLT_0D (uncertain) | m | Vertical full height | |
pf_active.coil[:].element[:].geometry.rectangle.r (alpha) | FLT_0D (uncertain) | m | Geometric centre R | |
pf_active.coil[:].element[:].geometry.rectangle.width (alpha) | FLT_0D (uncertain) | m | Horizontal full width | |
pf_active.coil[:].element[:].geometry.rectangle.z (alpha) | FLT_0D (uncertain) | m | Geometric centre Z | |
pf_active.coil[:].element[:].identifier (alpha) | STR_0D | Identifier of this element of this coil | ||
pf_active.coil[:].element[:].name (alpha) | STR_0D | Name of this element of this coil | ||
pf_active.coil[:].element[:].turns_with_sign (alpha) | INT_0D | Number of effective turns in the element for calculating magnetic fields of the coil; includes the sign of the number of turns | ||
pf_active.coil[:].energy_limit_max (alpha) | FLT_0D (uncertain) | J | Maximum Energy to be dissipated in the coil | |
pf_active.coil[:].identifier (alpha) | STR_0D | Alphanumeric identifier of coils used for convenience | ||
pf_active.coil[:].name (alpha) | STR_0D | Name of the coil | ||
pf_active.coil[:].resistance (alpha) | FLT_0D (uncertain) | Ohm | Coil resistance | |
pf_active.coil[:].voltage (alpha) | STRUCTURE | Voltage on the coil terminals | ||
pf_active.coil[:].voltage.data (alpha) | [pf_active.coil[:].voltage.time] | FLT_1D (uncertain) | V | Voltage on the coil terminals |
pf_active.coil[:].voltage.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pf_active.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
pf_active.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
pf_active.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
pf_active.ids_properties.occurrence | INT_0D | |||
pf_active.supply (alpha) | [1...N] | STRUCT_ARRAY | PF power supplies | |
pf_active.supply[:].current (alpha) | STRUCTURE | Current at the supply output, defined positive if it flows from point 1 to point 2 of the component in the pfcircuit description | ||
pf_active.supply[:].current.data (alpha) | [pf_active.supply[:].current.time] | FLT_1D (uncertain) | A | Current at the supply output, defined positive if it flows from point 1 to point 2 of the component in the pfcircuit description |
pf_active.supply[:].current.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pf_active.supply[:].current_limit_max (alpha) | FLT_0D (uncertain) | A | Maximum current in the supply | |
pf_active.supply[:].current_limit_min (alpha) | FLT_0D (uncertain) | A | Minimum current in the supply | |
pf_active.supply[:].current_limiter_gain (alpha) | FLT_0D (uncertain) | V | Gain to prevent overcurrent in a linear model of the supply | |
pf_active.supply[:].delay (alpha) | FLT_0D (uncertain) | s | Pure delay in the supply | |
pf_active.supply[:].energy_limit_max (alpha) | FLT_0D (uncertain) | J | Maximum energy to be dissipated in the supply during a pulse | |
pf_active.supply[:].filter_denominator (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Coefficients of the denominator, in increasing order : b0 + b1*s + ... + bm*s^m; used for a linear supply description |
pf_active.supply[:].filter_numerator (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Coefficients of the numerator, in increasing order : a0 + a1*s + ... + an*s^n; used for a linear supply description |
pf_active.supply[:].identifier (alpha) | STR_0D | Identifier of the supply | ||
pf_active.supply[:].name (alpha) | STR_0D | Name of the PF supply | ||
pf_active.supply[:].nonlinear_model (alpha) | STR_0D | Description of the nonlinear transfer function of the supply | ||
pf_active.supply[:].resistance (alpha) | FLT_0D (uncertain) | Ohm | Power supply internal resistance | |
pf_active.supply[:].type (alpha) | INT_0D | Type of the supply; TBD add free description of non-linear power supplies | ||
pf_active.supply[:].voltage (alpha) | STRUCTURE | Voltage at the supply output | ||
pf_active.supply[:].voltage.data (alpha) | [pf_active.supply[:].voltage.time] | FLT_1D (uncertain) | V | Voltage at the supply output |
pf_active.supply[:].voltage.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pf_active.supply[:].voltage_limit_max (alpha) | FLT_0D (uncertain) | V | Maximum voltage from the supply | |
pf_active.supply[:].voltage_limit_min (alpha) | FLT_0D (uncertain) | V | Minimum voltage from the supply | |
pf_active.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pf_active.vertical_force (alpha) | [1...N] | STRUCT_ARRAY | Vertical forces on the axisymmetric PF coil system | |
pf_active.vertical_force[:].combination (alpha) | [1...N] | FLT_1D (uncertain) | - | Coils involved in the force combinations. Normally the vertical force would be the full set of coils, but in some cases, we want to have a difference in forces, such as a CS coil separation force. We therefore give each coil a force weight which we call the combination |
pf_active.vertical_force[:].force (alpha) | STRUCTURE | Force | ||
pf_active.vertical_force[:].force.data (alpha) | [pf_active.vertical_force[:].force.time] | FLT_1D (uncertain) | N | Force |
pf_active.vertical_force[:].force.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pf_active.vertical_force[:].limit_max (alpha) | FLT_0D (uncertain) | N | Vertical force combination limit | |
pf_active.vertical_force[:].limit_min (alpha) | FLT_0D (uncertain) | N | Vertical force combination limit | |
pf_active.vertical_force[:].name (alpha) | STR_0D | Name of the force combination |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
pf_passive (alpha) | Description of the axisymmetric passive conductors, currents flowing in them | |||
pf_passive.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
pf_passive.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
pf_passive.code.name (alpha) | STR_0D | Name of software generating IDS | ||
pf_passive.code.output_flag (alpha) | [pf_passive.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
pf_passive.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
pf_passive.code.repository (alpha) | STR_0D | URL of software repository | ||
pf_passive.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
pf_passive.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
pf_passive.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
pf_passive.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
pf_passive.ids_properties.occurrence | INT_0D | |||
pf_passive.loop (alpha) | [1...N] | STRUCT_ARRAY | Passive axisymmetric conductor description in the form of non-connected loops; any connected loops are expressed as active coil circuits with no power supply attached. | |
pf_passive.loop[:].area (alpha) | FLT_0D (uncertain) | m^2 | Surface area of the passive loop | |
pf_passive.loop[:].current (alpha) | [pf_passive.time] | FLT_1D (uncertain) | A | Passive loop current |
pf_passive.loop[:].geometry (alpha) | STRUCTURE | Shape of the passive loop | ||
pf_passive.loop[:].geometry.geometry_type (alpha) | INT_0D | Type used to describe the element shape (1:'outline', 2:'rectangle', 3:'oblique') | ||
pf_passive.loop[:].geometry.oblique (alpha) | STRUCTURE | Trapezoidal description of the element | ||
pf_passive.loop[:].geometry.oblique.alpha (alpha) | FLT_0D (uncertain) | m | Inclination of first angle TBD | |
pf_passive.loop[:].geometry.oblique.beta (alpha) | FLT_0D (uncertain) | m | Inclination of second angle TBD | |
pf_passive.loop[:].geometry.oblique.length (alpha) | FLT_0D (uncertain) | m | Length | |
pf_passive.loop[:].geometry.oblique.r (alpha) | FLT_0D (uncertain) | m | Geometric centre R | |
pf_passive.loop[:].geometry.oblique.thickness (alpha) | FLT_0D (uncertain) | m | Thickness | |
pf_passive.loop[:].geometry.oblique.z (alpha) | FLT_0D (uncertain) | m | Geometric centre Z | |
pf_passive.loop[:].geometry.outline (alpha) | STRUCTURE | Irregular outline of the element | ||
pf_passive.loop[:].geometry.outline.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
pf_passive.loop[:].geometry.outline.z (alpha) | [pf_passive.loop[:].geometry.outline.r] | FLT_1D (uncertain) | m | Height |
pf_passive.loop[:].geometry.rectangle (alpha) | STRUCTURE | Rectangular description of the element | ||
pf_passive.loop[:].geometry.rectangle.height (alpha) | FLT_0D (uncertain) | m | Vertical full height | |
pf_passive.loop[:].geometry.rectangle.r (alpha) | FLT_0D (uncertain) | m | Geometric centre R | |
pf_passive.loop[:].geometry.rectangle.width (alpha) | FLT_0D (uncertain) | m | Horizontal full width | |
pf_passive.loop[:].geometry.rectangle.z (alpha) | FLT_0D (uncertain) | m | Geometric centre Z | |
pf_passive.loop[:].name (alpha) | STR_0D | Name of the loop | ||
pf_passive.loop[:].resistance (alpha) | FLT_0D (uncertain) | Ohm | Passive loop resistance | |
pf_passive.loop[:].resistivity (alpha) | FLT_0D (uncertain) | Ohm.m | Passive loop resistivity | |
pf_passive.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
pulse_schedule (alpha) | Description of Pulse Schedule, described by subsystems waveform references and an enveloppe aounrd them. The controllers, pulse schedule and SDN are defined separately | |||
pulse_schedule.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
pulse_schedule.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
pulse_schedule.code.name (alpha) | STR_0D | Name of software generating IDS | ||
pulse_schedule.code.output_flag (alpha) | [pulse_schedule.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
pulse_schedule.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
pulse_schedule.code.repository (alpha) | STR_0D | URL of software repository | ||
pulse_schedule.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
pulse_schedule.density_control (alpha) | STRUCTURE | Gas injection system and density control references | ||
pulse_schedule.density_control.mode (alpha) | STRUCTURE | Control mode (operation mode and/or settings used by the controller) | ||
pulse_schedule.density_control.mode.data (alpha) | [pulse_schedule.density_control.mode.time] | INT_1D | Control mode (operation mode and/or settings used by the controller) | |
pulse_schedule.density_control.mode.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.density_control.n_e_line (alpha) | STRUCTURE | m^-2 | Line integrated electron density | |
pulse_schedule.density_control.n_e_line.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.density_control.n_e_line.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.density_control.n_e_line.reference.data (alpha) | [pulse_schedule.density_control.n_e_line.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.density_control.n_e_line.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.density_control.n_e_line.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.density_control.n_e_line.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.density_control.n_h_over_n_d (alpha) | STRUCTURE | - | Average ratio of hydrogen over deuterium density | |
pulse_schedule.density_control.n_h_over_n_d.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.density_control.n_h_over_n_d.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.density_control.n_h_over_n_d.reference.data (alpha) | [pulse_schedule.density_control.n_h_over_n_d.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.density_control.n_h_over_n_d.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.density_control.n_h_over_n_d.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.density_control.n_h_over_n_d.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.density_control.n_t_over_n_d (alpha) | STRUCTURE | - | Average ratio of tritium over deuterium density | |
pulse_schedule.density_control.n_t_over_n_d.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.density_control.n_t_over_n_d.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.density_control.n_t_over_n_d.reference.data (alpha) | [pulse_schedule.density_control.n_t_over_n_d.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.density_control.n_t_over_n_d.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.density_control.n_t_over_n_d.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.density_control.n_t_over_n_d.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.density_control.valve (alpha) | [1...N] | STRUCT_ARRAY | Set of injection valves. Time-dependent | |
pulse_schedule.density_control.valve[:].flow_rate (alpha) | STRUCTURE | Pa.m^3.s^-1 | Flow rate of the valve | |
pulse_schedule.density_control.valve[:].flow_rate.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.density_control.valve[:].flow_rate.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.density_control.valve[:].flow_rate.reference.data (alpha) | [pulse_schedule.density_control.valve[:].flow_rate.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.density_control.valve[:].flow_rate.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.density_control.valve[:].flow_rate.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.density_control.valve[:].flow_rate.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.density_control.valve[:].species (alpha) | [1...N] | STRUCT_ARRAY | Species injected by the valve (may be more than one in case the valve injects a gas mixture) | |
pulse_schedule.density_control.valve[:].species[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
pulse_schedule.density_control.valve[:].species[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
pulse_schedule.density_control.valve[:].species[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
pulse_schedule.density_control.valve[:].species[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
pulse_schedule.density_control.valve[:].species[:].fraction (alpha) | INT_0D | Relative fraction of this species (in molecules) in the gas mixture | ||
pulse_schedule.density_control.valve[:].species[:].label (alpha) | STR_0D | String identifying neutral (e.g. H, D, T, He, C, ...) | ||
pulse_schedule.density_control.zeff (alpha) | STRUCTURE | - | Line average effective charge | |
pulse_schedule.density_control.zeff.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.density_control.zeff.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.density_control.zeff.reference.data (alpha) | [pulse_schedule.density_control.zeff.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.density_control.zeff.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.density_control.zeff.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.density_control.zeff.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ec (alpha) | STRUCTURE | Electron cyclotron heating and current drive system | ||
pulse_schedule.ec.antenna (alpha) | [1...N] | STRUCT_ARRAY | Set of ECRH antennas | |
pulse_schedule.ec.antenna[:].deposition_rho_tor_norm (alpha) | STRUCTURE | - | Normalised toroidal flux coordinate at which the main deposition should occur | |
pulse_schedule.ec.antenna[:].deposition_rho_tor_norm.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.ec.antenna[:].deposition_rho_tor_norm.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.ec.antenna[:].deposition_rho_tor_norm.reference.data (alpha) | [pulse_schedule.ec.antenna[:].deposition_rho_tor_norm.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.ec.antenna[:].deposition_rho_tor_norm.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ec.antenna[:].deposition_rho_tor_norm.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.ec.antenna[:].deposition_rho_tor_norm.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ec.antenna[:].frequency (alpha) | STRUCTURE | Hz | Frequency | |
pulse_schedule.ec.antenna[:].frequency.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.ec.antenna[:].frequency.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.ec.antenna[:].frequency.reference.data (alpha) | [pulse_schedule.ec.antenna[:].frequency.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.ec.antenna[:].frequency.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ec.antenna[:].frequency.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.ec.antenna[:].frequency.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ec.antenna[:].launching_angle_pol (alpha) | STRUCTURE | rad | Poloidal launching angle between the horizontal plane and the poloidal component of the nominal beam centerline. tan(angle_pol)=-k_z/k_R. Positive means wave launched downwards, negative means wave launched upwards | |
pulse_schedule.ec.antenna[:].launching_angle_pol.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.ec.antenna[:].launching_angle_pol.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.ec.antenna[:].launching_angle_pol.reference.data (alpha) | [pulse_schedule.ec.antenna[:].launching_angle_pol.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.ec.antenna[:].launching_angle_pol.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ec.antenna[:].launching_angle_pol.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.ec.antenna[:].launching_angle_pol.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ec.antenna[:].launching_angle_tor (alpha) | STRUCTURE | rad | Toroidal launching angle between the poloidal plane and the nominal beam centerline. sin(angle_tor)=k_phi. Positive sign means the waves is injected anti-clockwise when viewed from above. | |
pulse_schedule.ec.antenna[:].launching_angle_tor.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.ec.antenna[:].launching_angle_tor.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.ec.antenna[:].launching_angle_tor.reference.data (alpha) | [pulse_schedule.ec.antenna[:].launching_angle_tor.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.ec.antenna[:].launching_angle_tor.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ec.antenna[:].launching_angle_tor.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.ec.antenna[:].launching_angle_tor.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ec.antenna[:].phase (alpha) | STRUCTURE | rad | Phase | |
pulse_schedule.ec.antenna[:].phase.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.ec.antenna[:].phase.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.ec.antenna[:].phase.reference.data (alpha) | [pulse_schedule.ec.antenna[:].phase.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.ec.antenna[:].phase.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ec.antenna[:].phase.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.ec.antenna[:].phase.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ec.antenna[:].power (alpha) | STRUCTURE | W | Power | |
pulse_schedule.ec.antenna[:].power.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.ec.antenna[:].power.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.ec.antenna[:].power.reference.data (alpha) | [pulse_schedule.ec.antenna[:].power.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.ec.antenna[:].power.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ec.antenna[:].power.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.ec.antenna[:].power.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ec.mode (alpha) | STRUCTURE | Control mode (operation mode and/or settings used by the controller) | ||
pulse_schedule.ec.mode.data (alpha) | [pulse_schedule.ec.mode.time] | INT_1D | Control mode (operation mode and/or settings used by the controller) | |
pulse_schedule.ec.mode.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.flux_control (alpha) | STRUCTURE | Magnetic flux control references | ||
pulse_schedule.flux_control.beta_normal (alpha) | STRUCTURE | - | Normalised toroidal beta, defined as 100 * beta_tor * a[m] * B0 [T] / ip [MA] | |
pulse_schedule.flux_control.beta_normal.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.flux_control.beta_normal.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.flux_control.beta_normal.reference.data (alpha) | [pulse_schedule.flux_control.beta_normal.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.flux_control.beta_normal.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.flux_control.beta_normal.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.flux_control.beta_normal.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.flux_control.i_plasma (alpha) | STRUCTURE | A | Plasma current | |
pulse_schedule.flux_control.i_plasma.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.flux_control.i_plasma.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.flux_control.i_plasma.reference.data (alpha) | [pulse_schedule.flux_control.i_plasma.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.flux_control.i_plasma.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.flux_control.i_plasma.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.flux_control.i_plasma.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.flux_control.li_3 (alpha) | STRUCTURE | - | Internal inductance | |
pulse_schedule.flux_control.li_3.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.flux_control.li_3.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.flux_control.li_3.reference.data (alpha) | [pulse_schedule.flux_control.li_3.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.flux_control.li_3.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.flux_control.li_3.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.flux_control.li_3.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.flux_control.loop_voltage (alpha) | STRUCTURE | V | Loop voltage | |
pulse_schedule.flux_control.loop_voltage.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.flux_control.loop_voltage.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.flux_control.loop_voltage.reference.data (alpha) | [pulse_schedule.flux_control.loop_voltage.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.flux_control.loop_voltage.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.flux_control.loop_voltage.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.flux_control.loop_voltage.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.flux_control.mode (alpha) | STRUCTURE | Control mode (operation mode and/or settings used by the controller) | ||
pulse_schedule.flux_control.mode.data (alpha) | [pulse_schedule.flux_control.mode.time] | INT_1D | Control mode (operation mode and/or settings used by the controller) | |
pulse_schedule.flux_control.mode.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ic (alpha) | STRUCTURE | Ion cyclotron heating and current drive system | ||
pulse_schedule.ic.antenna (alpha) | [1...N] | STRUCT_ARRAY | Set of ICRH antennas | |
pulse_schedule.ic.antenna[:].frequency (alpha) | STRUCTURE | Hz | Frequency | |
pulse_schedule.ic.antenna[:].frequency.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.ic.antenna[:].frequency.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.ic.antenna[:].frequency.reference.data (alpha) | [pulse_schedule.ic.antenna[:].frequency.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.ic.antenna[:].frequency.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ic.antenna[:].frequency.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.ic.antenna[:].frequency.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ic.antenna[:].phase (alpha) | STRUCTURE | rad | Phase | |
pulse_schedule.ic.antenna[:].phase.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.ic.antenna[:].phase.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.ic.antenna[:].phase.reference.data (alpha) | [pulse_schedule.ic.antenna[:].phase.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.ic.antenna[:].phase.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ic.antenna[:].phase.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.ic.antenna[:].phase.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ic.antenna[:].power (alpha) | STRUCTURE | W | Power | |
pulse_schedule.ic.antenna[:].power.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.ic.antenna[:].power.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.ic.antenna[:].power.reference.data (alpha) | [pulse_schedule.ic.antenna[:].power.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.ic.antenna[:].power.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ic.antenna[:].power.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.ic.antenna[:].power.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.ic.mode (alpha) | STRUCTURE | Control mode (operation mode and/or settings used by the controller) | ||
pulse_schedule.ic.mode.data (alpha) | [pulse_schedule.ic.mode.time] | INT_1D | Control mode (operation mode and/or settings used by the controller) | |
pulse_schedule.ic.mode.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
pulse_schedule.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
pulse_schedule.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
pulse_schedule.ids_properties.occurrence | INT_0D | |||
pulse_schedule.lh (alpha) | STRUCTURE | Lower Hybrid heating and current drive system | ||
pulse_schedule.lh.antenna (alpha) | [1...N] | STRUCT_ARRAY | Set of LH antennas | |
pulse_schedule.lh.antenna[:].frequency (alpha) | STRUCTURE | Hz | Frequency | |
pulse_schedule.lh.antenna[:].frequency.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.lh.antenna[:].frequency.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.lh.antenna[:].frequency.reference.data (alpha) | [pulse_schedule.lh.antenna[:].frequency.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.lh.antenna[:].frequency.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.lh.antenna[:].frequency.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.lh.antenna[:].frequency.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.lh.antenna[:].n_parallel (alpha) | STRUCTURE | - | Main parallel refractive index of the injected wave power spectrum | |
pulse_schedule.lh.antenna[:].n_parallel.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.lh.antenna[:].n_parallel.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.lh.antenna[:].n_parallel.reference.data (alpha) | [pulse_schedule.lh.antenna[:].n_parallel.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.lh.antenna[:].n_parallel.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.lh.antenna[:].n_parallel.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.lh.antenna[:].n_parallel.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.lh.antenna[:].phase (alpha) | STRUCTURE | rad | Phasing between neighbour waveguides (in the toroidal direction) | |
pulse_schedule.lh.antenna[:].phase.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.lh.antenna[:].phase.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.lh.antenna[:].phase.reference.data (alpha) | [pulse_schedule.lh.antenna[:].phase.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.lh.antenna[:].phase.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.lh.antenna[:].phase.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.lh.antenna[:].phase.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.lh.antenna[:].power (alpha) | STRUCTURE | W | Power | |
pulse_schedule.lh.antenna[:].power.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.lh.antenna[:].power.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.lh.antenna[:].power.reference.data (alpha) | [pulse_schedule.lh.antenna[:].power.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.lh.antenna[:].power.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.lh.antenna[:].power.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.lh.antenna[:].power.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.lh.mode (alpha) | STRUCTURE | Control mode (operation mode and/or settings used by the controller) | ||
pulse_schedule.lh.mode.data (alpha) | [pulse_schedule.lh.mode.time] | INT_1D | Control mode (operation mode and/or settings used by the controller) | |
pulse_schedule.lh.mode.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.nbi (alpha) | STRUCTURE | Neutral beam heating and current drive system | ||
pulse_schedule.nbi.mode (alpha) | STRUCTURE | Control mode (operation mode and/or settings used by the controller) | ||
pulse_schedule.nbi.mode.data (alpha) | [pulse_schedule.nbi.mode.time] | INT_1D | Control mode (operation mode and/or settings used by the controller) | |
pulse_schedule.nbi.mode.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.nbi.unit (alpha) | [1...N] | STRUCT_ARRAY | Set of NBI units | |
pulse_schedule.nbi.unit[:].energy (alpha) | STRUCTURE | eV | Full energy of the injected species (acceleration of a single atom) | |
pulse_schedule.nbi.unit[:].energy.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.nbi.unit[:].energy.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.nbi.unit[:].energy.reference.data (alpha) | [pulse_schedule.nbi.unit[:].energy.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.nbi.unit[:].energy.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.nbi.unit[:].energy.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.nbi.unit[:].energy.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.nbi.unit[:].power (alpha) | STRUCTURE | W | Power | |
pulse_schedule.nbi.unit[:].power.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.nbi.unit[:].power.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.nbi.unit[:].power.reference.data (alpha) | [pulse_schedule.nbi.unit[:].power.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.nbi.unit[:].power.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.nbi.unit[:].power.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.nbi.unit[:].power.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.nbi.unit[:].species (alpha) | [1...N] | STRUCT_ARRAY | Species injected by the NBI unit (may be more than one in case the unit injects a gas mixture) | |
pulse_schedule.nbi.unit[:].species[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
pulse_schedule.nbi.unit[:].species[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
pulse_schedule.nbi.unit[:].species[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
pulse_schedule.nbi.unit[:].species[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
pulse_schedule.nbi.unit[:].species[:].fraction (alpha) | INT_0D | Relative fraction of this species (in molecules) in the gas mixture | ||
pulse_schedule.nbi.unit[:].species[:].label (alpha) | STR_0D | String identifying neutral (e.g. H, D, T, He, C, ...) | ||
pulse_schedule.position_control (alpha) | STRUCTURE | Plasma position and shape control references | ||
pulse_schedule.position_control.active_limiter_point (alpha) | STRUCTURE | RZ position of the active limiter point (point of the plasma boundary in contact with the limiter) | ||
pulse_schedule.position_control.active_limiter_point.r (alpha) | STRUCTURE | m | Major radius | |
pulse_schedule.position_control.active_limiter_point.r.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.active_limiter_point.r.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.active_limiter_point.r.reference.data (alpha) | [pulse_schedule.position_control.active_limiter_point.r.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.active_limiter_point.r.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.active_limiter_point.r.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.active_limiter_point.r.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.active_limiter_point.z (alpha) | STRUCTURE | m | Height | |
pulse_schedule.position_control.active_limiter_point.z.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.active_limiter_point.z.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.active_limiter_point.z.reference.data (alpha) | [pulse_schedule.position_control.active_limiter_point.z.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.active_limiter_point.z.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.active_limiter_point.z.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.active_limiter_point.z.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.boundary_outline (alpha) | [1...N] | STRUCT_ARRAY | Set of (R,Z) points defining the outline of the plasma boundary | |
pulse_schedule.position_control.boundary_outline[:].r (alpha) | STRUCTURE | m | Major radius | |
pulse_schedule.position_control.boundary_outline[:].r.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.boundary_outline[:].r.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.boundary_outline[:].r.reference.data (alpha) | [pulse_schedule.position_control.boundary_outline[:].r.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.boundary_outline[:].r.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.boundary_outline[:].r.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.boundary_outline[:].r.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.boundary_outline[:].z (alpha) | STRUCTURE | m | Height | |
pulse_schedule.position_control.boundary_outline[:].z.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.boundary_outline[:].z.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.boundary_outline[:].z.reference.data (alpha) | [pulse_schedule.position_control.boundary_outline[:].z.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.boundary_outline[:].z.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.boundary_outline[:].z.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.boundary_outline[:].z.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.elongation (alpha) | STRUCTURE | - | Elongation of the plasma boundary | |
pulse_schedule.position_control.elongation.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.elongation.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.elongation.reference.data (alpha) | [pulse_schedule.position_control.elongation.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.elongation.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.elongation.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.elongation.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.elongation_lower (alpha) | STRUCTURE | - | Elongation (lower half w.r.t. geometric axis) of the plasma boundary | |
pulse_schedule.position_control.elongation_lower.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.elongation_lower.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.elongation_lower.reference.data (alpha) | [pulse_schedule.position_control.elongation_lower.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.elongation_lower.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.elongation_lower.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.elongation_lower.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.elongation_upper (alpha) | STRUCTURE | - | Elongation (upper half w.r.t. geometric axis) of the plasma boundary | |
pulse_schedule.position_control.elongation_upper.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.elongation_upper.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.elongation_upper.reference.data (alpha) | [pulse_schedule.position_control.elongation_upper.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.elongation_upper.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.elongation_upper.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.elongation_upper.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.gap (alpha) | [1...N] | STRUCT_ARRAY | Set of gaps, defined by a reference point and a direction. | |
pulse_schedule.position_control.gap[:].angle (alpha) | FLT_0D (uncertain) | rad | Angle between the direction in which the gap is measured (in the poloidal cross-section) and the horizontal axis. | |
pulse_schedule.position_control.gap[:].r (alpha) | FLT_0D (uncertain) | m | Major radius of the reference point | |
pulse_schedule.position_control.gap[:].value (alpha) | STRUCTURE | m | Value of the gap, i.e. distance between the reference point and the separatrix along the gap direction | |
pulse_schedule.position_control.gap[:].value.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.gap[:].value.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.gap[:].value.reference.data (alpha) | [pulse_schedule.position_control.gap[:].value.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.gap[:].value.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.gap[:].value.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.gap[:].value.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.gap[:].z (alpha) | FLT_0D (uncertain) | m | Height of the reference point | |
pulse_schedule.position_control.geometric_axis (alpha) | STRUCTURE | RZ position of the geometric axis (defined as (Rmin+Rmax) / 2 and (Zmin+Zmax) / 2 of the boundary) | ||
pulse_schedule.position_control.geometric_axis.r (alpha) | STRUCTURE | m | Major radius | |
pulse_schedule.position_control.geometric_axis.r.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.geometric_axis.r.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.geometric_axis.r.reference.data (alpha) | [pulse_schedule.position_control.geometric_axis.r.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.geometric_axis.r.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.geometric_axis.r.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.geometric_axis.r.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.geometric_axis.z (alpha) | STRUCTURE | m | Height | |
pulse_schedule.position_control.geometric_axis.z.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.geometric_axis.z.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.geometric_axis.z.reference.data (alpha) | [pulse_schedule.position_control.geometric_axis.z.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.geometric_axis.z.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.geometric_axis.z.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.geometric_axis.z.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.magnetic_axis (alpha) | STRUCTURE | Magnetic axis position | ||
pulse_schedule.position_control.magnetic_axis.r (alpha) | STRUCTURE | m | Major radius | |
pulse_schedule.position_control.magnetic_axis.r.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.magnetic_axis.r.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.magnetic_axis.r.reference.data (alpha) | [pulse_schedule.position_control.magnetic_axis.r.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.magnetic_axis.r.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.magnetic_axis.r.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.magnetic_axis.r.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.magnetic_axis.z (alpha) | STRUCTURE | m | Height | |
pulse_schedule.position_control.magnetic_axis.z.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.magnetic_axis.z.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.magnetic_axis.z.reference.data (alpha) | [pulse_schedule.position_control.magnetic_axis.z.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.magnetic_axis.z.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.magnetic_axis.z.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.magnetic_axis.z.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.minor_radius (alpha) | STRUCTURE | m | Minor radius of the plasma boundary (defined as (Rmax-Rmin) / 2 of the boundary) | |
pulse_schedule.position_control.minor_radius.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.minor_radius.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.minor_radius.reference.data (alpha) | [pulse_schedule.position_control.minor_radius.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.minor_radius.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.minor_radius.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.minor_radius.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.mode (alpha) | STRUCTURE | Control mode (operation mode and/or settings used by the controller) | ||
pulse_schedule.position_control.mode.data (alpha) | [pulse_schedule.position_control.mode.time] | INT_1D | Control mode (operation mode and/or settings used by the controller) | |
pulse_schedule.position_control.mode.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.strike_point (alpha) | [1...N] | STRUCT_ARRAY | Array of strike points, for each of them the RZ position is given | |
pulse_schedule.position_control.strike_point[:].r (alpha) | STRUCTURE | m | Major radius | |
pulse_schedule.position_control.strike_point[:].r.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.strike_point[:].r.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.strike_point[:].r.reference.data (alpha) | [pulse_schedule.position_control.strike_point[:].r.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.strike_point[:].r.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.strike_point[:].r.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.strike_point[:].r.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.strike_point[:].z (alpha) | STRUCTURE | m | Height | |
pulse_schedule.position_control.strike_point[:].z.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.strike_point[:].z.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.strike_point[:].z.reference.data (alpha) | [pulse_schedule.position_control.strike_point[:].z.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.strike_point[:].z.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.strike_point[:].z.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.strike_point[:].z.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.triangularity (alpha) | STRUCTURE | - | Triangularity of the plasma boundary | |
pulse_schedule.position_control.triangularity.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.triangularity.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.triangularity.reference.data (alpha) | [pulse_schedule.position_control.triangularity.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.triangularity.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.triangularity.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.triangularity.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.triangularity_lower (alpha) | STRUCTURE | - | Lower triangularity of the plasma boundary | |
pulse_schedule.position_control.triangularity_lower.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.triangularity_lower.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.triangularity_lower.reference.data (alpha) | [pulse_schedule.position_control.triangularity_lower.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.triangularity_lower.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.triangularity_lower.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.triangularity_lower.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.triangularity_upper (alpha) | STRUCTURE | - | Upper triangularity of the plasma boundary | |
pulse_schedule.position_control.triangularity_upper.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.triangularity_upper.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.triangularity_upper.reference.data (alpha) | [pulse_schedule.position_control.triangularity_upper.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.triangularity_upper.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.triangularity_upper.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.triangularity_upper.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.x_point (alpha) | [1...N] | STRUCT_ARRAY | Array of X-points, for each of them the RZ position is given | |
pulse_schedule.position_control.x_point[:].r (alpha) | STRUCTURE | m | Major radius | |
pulse_schedule.position_control.x_point[:].r.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.x_point[:].r.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.x_point[:].r.reference.data (alpha) | [pulse_schedule.position_control.x_point[:].r.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.x_point[:].r.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.x_point[:].r.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.x_point[:].r.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.position_control.x_point[:].z (alpha) | STRUCTURE | m | Height | |
pulse_schedule.position_control.x_point[:].z.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.position_control.x_point[:].z.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.position_control.x_point[:].z.reference.data (alpha) | [pulse_schedule.position_control.x_point[:].z.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.position_control.x_point[:].z.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.position_control.x_point[:].z.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.position_control.x_point[:].z.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.tf (alpha) | STRUCTURE | Toroidal field references | ||
pulse_schedule.tf.b_field_tor_vacuum_r (alpha) | STRUCTURE | T.m | Vacuum field times major radius in the toroidal field magnet. Positive sign means anti-clockwise when viewed from above | |
pulse_schedule.tf.b_field_tor_vacuum_r.envelope_type (alpha) | INT_0D | Envelope type: 0:relative; 1: absolute; refers to the envelope bounds which are given by the reference/data_error_upper and reference/data_error_lower nodes | ||
pulse_schedule.tf.b_field_tor_vacuum_r.reference (alpha) | STRUCTURE | Reference waveform | ||
pulse_schedule.tf.b_field_tor_vacuum_r.reference.data (alpha) | [pulse_schedule.tf.b_field_tor_vacuum_r.reference.time] | FLT_1D (uncertain) | mixed | Reference waveform |
pulse_schedule.tf.b_field_tor_vacuum_r.reference.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.tf.b_field_tor_vacuum_r.reference_name (alpha) | STR_0D | Reference name (e.g. in the native pulse schedule system of the device) | ||
pulse_schedule.tf.b_field_tor_vacuum_r.reference_type (alpha) | INT_0D | Reference type: 0:relative; 1: absolute; refers to the reference/data node | ||
pulse_schedule.tf.mode (alpha) | STRUCTURE | Control mode (operation mode and/or settings used by the controller) | ||
pulse_schedule.tf.mode.data (alpha) | [pulse_schedule.tf.mode.time] | INT_1D | Control mode (operation mode and/or settings used by the controller) | |
pulse_schedule.tf.mode.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
pulse_schedule.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
sawteeth (alpha) | Description of sawtooth events. This IDS must be used in homogeneous_time = 1 mode | |||
sawteeth.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
sawteeth.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
sawteeth.code.name (alpha) | STR_0D | Name of software generating IDS | ||
sawteeth.code.output_flag (alpha) | [sawteeth.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
sawteeth.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
sawteeth.code.repository (alpha) | STR_0D | URL of software repository | ||
sawteeth.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
sawteeth.crash_trigger (alpha) | [sawteeth.time] | INT_1D | Flag indicating whether a crash condition has been satisfied : 0 = no crash. N(>0) = crash triggered due to condition N as follows. 1: crash triggered by the ideal kink criterion; 2: crash triggered by the ideal kink criterion including kinetic effects from fast particles; 31: crash triggered by the resistive kink criterion (meeting necessary conditions for reconnection); 32: crash triggered by the resistive kink criterion (resistive kink mode is unstable). The distinction between 31 and 32 only indicates whether (31) or (32) was the last criterion to be satisfied | |
sawteeth.diagnostics (alpha) | STRUCTURE | Detailed information about the sawtooth characteristics | ||
sawteeth.diagnostics.magnetic_shear_q1 (alpha) | [sawteeth.time] | FLT_1D (uncertain) | - | Magnetic shear at surface q = 1, defined as rho_tor/q . dq/drho_tor |
sawteeth.diagnostics.previous_crash_time (alpha) | [sawteeth.time] | FLT_1D (uncertain) | s | Time at which the previous sawtooth crash occured |
sawteeth.diagnostics.previous_crash_trigger (alpha) | [sawteeth.time] | INT_1D | Previous crash trigger. Flag indicating whether a crash condition has been satisfied : 0 = no crash. N(>0) = crash triggered due to condition N | |
sawteeth.diagnostics.previous_period (alpha) | [sawteeth.time] | FLT_1D (uncertain) | s | Previous sawtooth period |
sawteeth.diagnostics.rho_tor_norm_inversion (alpha) | [sawteeth.time] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate at inversion radius |
sawteeth.diagnostics.rho_tor_norm_mixing (alpha) | [sawteeth.time] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate at mixing radius |
sawteeth.diagnostics.rho_tor_norm_q1 (alpha) | [sawteeth.time] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate at surface q = 1 |
sawteeth.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
sawteeth.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
sawteeth.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
sawteeth.ids_properties.occurrence | INT_0D | |||
sawteeth.profiles_1d (alpha) | [sawteeth.profiles_1d[:].time] | STRUCT_ARRAY | Core profiles after sawtooth crash for various time slices | |
sawteeth.profiles_1d[:].conductivity_parallel (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | ohm^-1.m^-1 | Parallel conductivity |
sawteeth.profiles_1d[:].e_field_parallel (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Parallel electric field = average(E.B) / B0, where Core_Profiles/Vacuum_Toroidal_Field/ B0 |
sawteeth.profiles_1d[:].grid (alpha) | STRUCTURE | Radial grid | ||
sawteeth.profiles_1d[:].grid.area (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
sawteeth.profiles_1d[:].grid.psi (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
sawteeth.profiles_1d[:].grid.rho_tor (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
sawteeth.profiles_1d[:].grid.rho_tor_norm (alpha) | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
sawteeth.profiles_1d[:].grid.volume (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
sawteeth.profiles_1d[:].j_bootstrap (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Bootstrap current density = average(J_Bootstrap.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
sawteeth.profiles_1d[:].j_non_inductive (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Non-inductive (includes bootstrap) parallel current density = average(jni.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
sawteeth.profiles_1d[:].j_ohmic (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Ohmic parallel current density = average(J_Ohmic.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
sawteeth.profiles_1d[:].j_tor (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Total toroidal current density = average(J_Tor/R) / average(1/R) |
sawteeth.profiles_1d[:].j_total (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A/m^2 | Total parallel current density = average(jtot.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0 |
sawteeth.profiles_1d[:].magnetic_shear (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor |
sawteeth.profiles_1d[:].momentum_tor (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | kg.m/s | Total plasma toroidal momentum, summed over ion species and electrons |
sawteeth.profiles_1d[:].n_e (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Electron density (thermal+non-thermal) |
sawteeth.profiles_1d[:].n_e_fast (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) electrons |
sawteeth.profiles_1d[:].n_i_total_over_n_e (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal) |
sawteeth.profiles_1d[:].p_e (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Electron pressure |
sawteeth.profiles_1d[:].p_e_fast_parallel (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) electron parallel pressure |
sawteeth.profiles_1d[:].p_e_fast_perpendicular (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) electron perpendicular pressure |
sawteeth.profiles_1d[:].p_i_total (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total ion pressure (sum over the ion species) |
sawteeth.profiles_1d[:].p_i_total_fast_parallel (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) total ion (sum over the ion species) parallel pressure |
sawteeth.profiles_1d[:].p_i_total_fast_perpendicular (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) total ion (sum over the ion species) perpendicular pressure |
sawteeth.profiles_1d[:].phi (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Toroidal flux |
sawteeth.profiles_1d[:].pressure_parallel (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total parallel pressure (electrons+ions, thermal+non-thermal) |
sawteeth.profiles_1d[:].pressure_perpendicular (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total perpendicular pressure (electrons+ions, thermal+non-thermal) |
sawteeth.profiles_1d[:].pressure_thermal (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Thermal pressure (electrons+ions) |
sawteeth.profiles_1d[:].psi_star_post_crash (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Psi* = psi - phi, after the sawtooth crash |
sawteeth.profiles_1d[:].psi_star_pre_crash (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Psi* = psi - phi, just before the sawtooth crash |
sawteeth.profiles_1d[:].q (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Safety factor |
sawteeth.profiles_1d[:].t_e (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Electron temperature |
sawteeth.profiles_1d[:].t_i_average (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Ion temperature (averaged on charge states and ion species) |
sawteeth.profiles_1d[:].time (alpha) | FLT_0D | s | Time | |
sawteeth.profiles_1d[:].zeff (alpha) | [sawteeth.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Effective charge |
sawteeth.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
sawteeth.vacuum_toroidal_field (alpha) | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition) | ||
sawteeth.vacuum_toroidal_field.b0 (alpha) | [sawteeth.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
sawteeth.vacuum_toroidal_field.r0 (alpha) | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
sdn (alpha) | Description of the Synchronous Data Network parameters and the signals on it | |||
sdn.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
sdn.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
sdn.code.name (alpha) | STR_0D | Name of software generating IDS | ||
sdn.code.output_flag (alpha) | [sdn.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
sdn.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
sdn.code.repository (alpha) | STR_0D | URL of software repository | ||
sdn.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
sdn.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
sdn.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
sdn.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
sdn.ids_properties.occurrence | INT_0D | |||
sdn.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
sdn.topic (alpha) | [1...N] | STRUCT_ARRAY | List of topics. SDN signals are grouped by topic | |
sdn.topic[:].name (alpha) | STR_0D | Topic name | ||
sdn.topic[:].signal (alpha) | [1...N] | STRUCT_ARRAY | List of signals which can be allocated to the SDN | |
sdn.topic[:].signal[:].allocated_position (alpha) | INT_0D | Allocation of signal to a position in the SDN (1..N); this will be implementation specific | ||
sdn.topic[:].signal[:].definition (alpha) | STR_0D | Signal definition | ||
sdn.topic[:].signal[:].name (alpha) | STR_0D | Signal name | ||
sdn.topic[:].signal[:].quality (alpha) | STRUCTURE | Indicator of the quality of the signal. Following ITER PCS documentation (https://user.iter.org/?uid=354SJ3&action=get_document), possible values are: 1 - GOOD (the nominal state); 2 - INVALID (data no usable); 3 - DATA INTEGRITY ERROR (e.g. out of bounds with respect to expectations, calibration error,...) | ||
sdn.topic[:].signal[:].quality.data (alpha) | [sdn.topic[:].signal[:].quality.time] | INT_1D | Indicator of the quality of the signal. Following ITER PCS documentation (https://user.iter.org/?uid=354SJ3&action=get_document), possible values are: 1 - GOOD (the nominal state); 2 - INVALID (data no usable); 3 - DATA INTEGRITY ERROR (e.g. out of bounds with respect to expectations, calibration error,...) | |
sdn.topic[:].signal[:].quality.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
sdn.topic[:].signal[:].value (alpha) | STRUCTURE | Signal value | ||
sdn.topic[:].signal[:].value.data (alpha) | [sdn.topic[:].signal[:].value.time] | FLT_1D (uncertain) | mixed | Signal value |
sdn.topic[:].signal[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
spectrometer_visible (alpha) | Spectrometer in visible light range diagnostic | |||
spectrometer_visible.channel (alpha) | [1...N] | STRUCT_ARRAY | Set of channels (lines-of-sight) | |
spectrometer_visible.channel[:].filter (alpha) | STRUCTURE | Quantities measured by the channel if connected to a filter spectrometer | ||
spectrometer_visible.channel[:].filter.calibrated_line_integrals (alpha) | STRUCTURE | Calibrated line gross areas integrals | ||
spectrometer_visible.channel[:].filter.calibrated_line_integrals.data (alpha) | [spectrometer_visible.channel[:].filter.calibrated_lines, | FLT_2D (uncertain) | m^-2.s^-1.sr^-1 | Calibrated line gross areas integrals |
spectrometer_visible.channel[:].filter.calibrated_line_integrals.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
spectrometer_visible.channel[:].filter.calibrated_lines (alpha) | [1...N] | FLT_1D (uncertain) | m | Central wavelength of the calibrated lines |
spectrometer_visible.channel[:].filter.exposure_time (alpha) | FLT_0D (uncertain) | s | Exposure time | |
spectrometer_visible.channel[:].filter.line_intensities (alpha) | STRUCTURE | Line gross integral intensities | ||
spectrometer_visible.channel[:].filter.line_intensities.data (alpha) | [spectrometer_visible.channel[:].filter.raw_lines, | FLT_2D (uncertain) | m^-2.s^-1.sr^-1 | Line gross integral intensities |
spectrometer_visible.channel[:].filter.line_intensities.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
spectrometer_visible.channel[:].filter.line_radiances (alpha) | STRUCTURE | Calibrated, background subtracted line integrals | ||
spectrometer_visible.channel[:].filter.line_radiances.data (alpha) | [spectrometer_visible.channel[:].filter.processed_lines, | FLT_2D (uncertain) | m^-2.s^-1.sr^-1 | Calibrated, background subtracted line integrals |
spectrometer_visible.channel[:].filter.line_radiances.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
spectrometer_visible.channel[:].filter.processed_lines (alpha) | [1...N] | FLT_1D (uncertain) | m | Central wavelength of the processed lines |
spectrometer_visible.channel[:].filter.radiance_calibration (alpha) | FLT_0D (uncertain) | m^-2.sr^-1 | Radiance calibration | |
spectrometer_visible.channel[:].filter.radiance_calibration_date (alpha) | STR_0D | Date of the radiance calibration (yyyy_mm_dd) | ||
spectrometer_visible.channel[:].filter.raw_lines (alpha) | [1...N] | FLT_1D (uncertain) | m | Central wavelength of the raw lines |
spectrometer_visible.channel[:].grating (alpha) | STRUCTURE | Quantities measured by the channel if connected to a grating spectrometer | ||
spectrometer_visible.channel[:].grating.exposure_time (alpha) | FLT_0D (uncertain) | s | Exposure time | |
spectrometer_visible.channel[:].grating.intensity_spectra (alpha) | STRUCTURE | Intensity spectra (not calibrated) | ||
spectrometer_visible.channel[:].grating.intensity_spectra.data (alpha) | [spectrometer_visible.channel[:].grating.wavelengths, | FLT_2D (uncertain) | s^-1 | Intensity spectra (not calibrated) |
spectrometer_visible.channel[:].grating.intensity_spectra.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
spectrometer_visible.channel[:].grating.line_radiances (alpha) | STRUCTURE | Calibrated, background subtracted line integrals | ||
spectrometer_visible.channel[:].grating.line_radiances.data (alpha) | [spectrometer_visible.channel[:].grating.processed_lines, | FLT_2D (uncertain) | m^-2.s^-1.sr^-1 | Calibrated, background subtracted line integrals |
spectrometer_visible.channel[:].grating.line_radiances.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
spectrometer_visible.channel[:].grating.processed_lines (alpha) | [1...N] | FLT_1D (uncertain) | m | Central wavelength of the processed lines |
spectrometer_visible.channel[:].grating.radiance_calibration (alpha) | [spectrometer_visible.channel[:].grating.wavelengths] | FLT_1D (uncertain) | m^-2.sr^-1 | Radiance calibration |
spectrometer_visible.channel[:].grating.radiance_calibration_date (alpha) | STR_0D | Date of the radiance calibration (yyyy_mm_dd) | ||
spectrometer_visible.channel[:].grating.radiance_spectra (alpha) | STRUCTURE | Calibrated spectra | ||
spectrometer_visible.channel[:].grating.radiance_spectra.data (alpha) | [spectrometer_visible.channel[:].grating.wavelengths, | FLT_2D (uncertain) | m^-2.s^-1.sr^-1 | Calibrated spectra |
spectrometer_visible.channel[:].grating.radiance_spectra.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
spectrometer_visible.channel[:].grating.wavelength_calibration_date (alpha) | STR_0D | Date of the wavelength calibration (yyyy_mm_dd) | ||
spectrometer_visible.channel[:].grating.wavelengths (alpha) | [1...N] | FLT_1D (uncertain) | m | Measured wavelengths |
spectrometer_visible.channel[:].line_of_sight (alpha) | STRUCTURE | Description of the line of sight of the channel, given by 2 points | ||
spectrometer_visible.channel[:].line_of_sight.first_point (alpha) | STRUCTURE | Position of the first point | ||
spectrometer_visible.channel[:].line_of_sight.first_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
spectrometer_visible.channel[:].line_of_sight.first_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
spectrometer_visible.channel[:].line_of_sight.first_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
spectrometer_visible.channel[:].line_of_sight.second_point (alpha) | STRUCTURE | Position of the second point | ||
spectrometer_visible.channel[:].line_of_sight.second_point.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
spectrometer_visible.channel[:].line_of_sight.second_point.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
spectrometer_visible.channel[:].line_of_sight.second_point.z (alpha) | FLT_0D (uncertain) | m | Height | |
spectrometer_visible.channel[:].name (alpha) | STR_0D | Name of the channel | ||
spectrometer_visible.channel[:].spot_diameter (alpha) | FLT_0D (uncertain) | m | Spot diameter | |
spectrometer_visible.channel[:].type (alpha) | STRUCTURE | Type of spectrometer the channel is connected to (index=1: grating, 2: filter) | ||
spectrometer_visible.channel[:].type.description (alpha) | STR_0D | Verbose description | ||
spectrometer_visible.channel[:].type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
spectrometer_visible.channel[:].type.name (alpha) | STR_0D | Short string identifier | ||
spectrometer_visible.channel[:].validity (alpha) | INT_0D | Indicator of the validity of the channel for the whole acquisition period (0 means valid, negative values mean non-valid) | ||
spectrometer_visible.channel[:].validity_timed (alpha) | STRUCTURE | Indicator of the validity of the channel as a function of time (0 means valid, negative values mean non-valid) | ||
spectrometer_visible.channel[:].validity_timed.data (alpha) | [spectrometer_visible.channel[:].validity_timed.time] | INT_1D | Indicator of the validity of the channel as a function of time (0 means valid, negative values mean non-valid) | |
spectrometer_visible.channel[:].validity_timed.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
spectrometer_visible.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
spectrometer_visible.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
spectrometer_visible.code.name (alpha) | STR_0D | Name of software generating IDS | ||
spectrometer_visible.code.output_flag (alpha) | [spectrometer_visible.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
spectrometer_visible.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
spectrometer_visible.code.repository (alpha) | STR_0D | URL of software repository | ||
spectrometer_visible.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
spectrometer_visible.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
spectrometer_visible.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
spectrometer_visible.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
spectrometer_visible.ids_properties.occurrence | INT_0D | |||
spectrometer_visible.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
summary (alpha) | Summary of physics quantities from a simulation or an experiment | |||
summary.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
summary.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
summary.code.name (alpha) | STR_0D | Name of software generating IDS | ||
summary.code.output_flag (alpha) | [summary.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
summary.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
summary.code.repository (alpha) | STR_0D | URL of software repository | ||
summary.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
summary.disruption (alpha) | STRUCTURE | Disruption characteristics, if the pulse is terminated by a disruption | ||
summary.disruption.mitigation_valve (alpha) | STRUCTURE | Flag indicating whether any disruption mitigation valve has been used (1) or none (0) | ||
summary.disruption.mitigation_valve.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.disruption.mitigation_valve.value (alpha) | INT_0D | ? | Value | |
summary.disruption.time (alpha) | STRUCTURE | s | Time of the disruption | |
summary.disruption.time.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.disruption.time.value (alpha) | FLT_0D (uncertain) | s | Value | |
summary.disruption.time_half_ip (alpha) | STRUCTURE | s | Time at which the plasma current has fallen to half of the initial current at the start of the disruption, relative to the time of the disruption | |
summary.disruption.time_half_ip.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.disruption.time_half_ip.value (alpha) | FLT_0D (uncertain) | s | Value | |
summary.disruption.time_radiated_power_max (alpha) | STRUCTURE | s | Time of maximum radiated power, relative to the time of the disruption | |
summary.disruption.time_radiated_power_max.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.disruption.time_radiated_power_max.value (alpha) | FLT_0D (uncertain) | s | Value | |
summary.disruption.vertical_displacement (alpha) | STRUCTURE | s | Direction of the plasma vertical displacement just before the disruption 1 (upwards) / 0 (no displacement)/ -1 (downwards) | |
summary.disruption.vertical_displacement.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.disruption.vertical_displacement.value (alpha) | INT_0D | s | Value | |
summary.fusion (alpha) | STRUCTURE | Fusion reactions | ||
summary.fusion.current (alpha) | STRUCTURE | A | Parallel current driven by this fusion reactions | |
summary.fusion.current.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.current.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.fusion.neutron_fluxes (alpha) | STRUCTURE | Neutron fluxes from various reactions | ||
summary.fusion.neutron_fluxes.dd (alpha) | STRUCTURE | Neutron fluxes from DD reactions | ||
summary.fusion.neutron_fluxes.dd.beam_beam (alpha) | STRUCTURE | Hz | Neutron flux coming from NBI beam self reactions | |
summary.fusion.neutron_fluxes.dd.beam_beam.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.dd.beam_beam.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.dd.beam_thermal (alpha) | STRUCTURE | Hz | Neutron flux coming from NBI beam - plasma reactions | |
summary.fusion.neutron_fluxes.dd.beam_thermal.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.dd.beam_thermal.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.dd.thermal (alpha) | STRUCTURE | Hz | Neutron flux coming from thermal plasma | |
summary.fusion.neutron_fluxes.dd.thermal.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.dd.thermal.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.dd.total (alpha) | STRUCTURE | Hz | Total neutron flux coming from this reaction | |
summary.fusion.neutron_fluxes.dd.total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.dd.total.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.dt (alpha) | STRUCTURE | Neutron fluxes from DT reactions | ||
summary.fusion.neutron_fluxes.dt.beam_beam (alpha) | STRUCTURE | Hz | Neutron flux coming from NBI beam self reactions | |
summary.fusion.neutron_fluxes.dt.beam_beam.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.dt.beam_beam.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.dt.beam_thermal (alpha) | STRUCTURE | Hz | Neutron flux coming from NBI beam - plasma reactions | |
summary.fusion.neutron_fluxes.dt.beam_thermal.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.dt.beam_thermal.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.dt.thermal (alpha) | STRUCTURE | Hz | Neutron flux coming from thermal plasma | |
summary.fusion.neutron_fluxes.dt.thermal.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.dt.thermal.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.dt.total (alpha) | STRUCTURE | Hz | Total neutron flux coming from this reaction | |
summary.fusion.neutron_fluxes.dt.total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.dt.total.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.thermal (alpha) | STRUCTURE | Hz | Neutron flux from all plasma thermal reactions | |
summary.fusion.neutron_fluxes.thermal.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.thermal.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.total (alpha) | STRUCTURE | Hz | Total neutron flux from all reactions | |
summary.fusion.neutron_fluxes.total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.total.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.tt (alpha) | STRUCTURE | Neutron fluxes from TT reactions | ||
summary.fusion.neutron_fluxes.tt.beam_beam (alpha) | STRUCTURE | Hz | Neutron flux coming from NBI beam self reactions | |
summary.fusion.neutron_fluxes.tt.beam_beam.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.tt.beam_beam.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.tt.beam_thermal (alpha) | STRUCTURE | Hz | Neutron flux coming from NBI beam - plasma reactions | |
summary.fusion.neutron_fluxes.tt.beam_thermal.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.tt.beam_thermal.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.tt.thermal (alpha) | STRUCTURE | Hz | Neutron flux coming from thermal plasma | |
summary.fusion.neutron_fluxes.tt.thermal.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.tt.thermal.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.neutron_fluxes.tt.total (alpha) | STRUCTURE | Hz | Total neutron flux coming from this reaction | |
summary.fusion.neutron_fluxes.tt.total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.neutron_fluxes.tt.total.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.fusion.power (alpha) | STRUCTURE | W | Power coupled to the plasma by fusion reactions | |
summary.fusion.power.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.fusion.power.value (alpha) | [summary.time] | FLT_1D (uncertain) | W | Value |
summary.global_quantities (alpha) | STRUCTURE | Various global quantities derived from the profiles | ||
summary.global_quantities.b0 (alpha) | STRUCTURE | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. | |
summary.global_quantities.b0.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.b0.value (alpha) | [summary.time] | FLT_1D (uncertain) | T | Value |
summary.global_quantities.beta_pol (alpha) | STRUCTURE | - | Poloidal beta. Defined as betap = 4 int(p dV) / [R_0 * mu_0 * Ip^2] | |
summary.global_quantities.beta_pol.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.beta_pol.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.global_quantities.beta_tor (alpha) | STRUCTURE | - | Toroidal beta, defined as the volume-averaged total perpendicular pressure divided by (B0^2/(2*mu0)), i.e. beta_toroidal = 2 mu0 int(p dV) / V / B0^2 | |
summary.global_quantities.beta_tor.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.beta_tor.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.global_quantities.beta_tor_norm (alpha) | STRUCTURE | - | Normalised toroidal beta, defined as 100 * beta_tor * a[m] * B0 [T] / ip [MA] | |
summary.global_quantities.beta_tor_norm.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.beta_tor_norm.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.global_quantities.current_alignment (alpha) | STRUCTURE | A | Figure of merit of the alignment of the current profile sources, defined in the following reference: http://iopscience.iop.org/article/10.1088/0029-5515/43/7/318 | |
summary.global_quantities.current_alignment.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.current_alignment.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.global_quantities.current_bootstrap (alpha) | STRUCTURE | A | Bootstrap parallel current | |
summary.global_quantities.current_bootstrap.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.current_bootstrap.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.global_quantities.current_non_inductive (alpha) | STRUCTURE | A | Total non-inductive parallel current | |
summary.global_quantities.current_non_inductive.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.current_non_inductive.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.global_quantities.current_ohm (alpha) | STRUCTURE | A | Ohmic parallel current | |
summary.global_quantities.current_ohm.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.current_ohm.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.global_quantities.energy_b_field_pol (alpha) | STRUCTURE | J | Thermal plasma energy content = 1/(2.mu0) * integral over the plasma volume of b_field_pol^2 | |
summary.global_quantities.energy_b_field_pol.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.energy_b_field_pol.value (alpha) | [summary.time] | FLT_1D (uncertain) | J | Value |
summary.global_quantities.energy_diamagnetic (alpha) | STRUCTURE | J | Plasma energy content = 3/2 * integral over the plasma volume of the total perpendicular pressure | |
summary.global_quantities.energy_diamagnetic.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.energy_diamagnetic.value (alpha) | [summary.time] | FLT_1D (uncertain) | J | Value |
summary.global_quantities.energy_thermal (alpha) | STRUCTURE | J | Thermal plasma energy content = 3/2 * integral over the plasma volume of the thermal pressure | |
summary.global_quantities.energy_thermal.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.energy_thermal.value (alpha) | [summary.time] | FLT_1D (uncertain) | J | Value |
summary.global_quantities.energy_total (alpha) | STRUCTURE | J | Plasma energy content = 3/2 * integral over the plasma volume of the total kinetic pressure | |
summary.global_quantities.energy_total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.energy_total.value (alpha) | [summary.time] | FLT_1D (uncertain) | J | Value |
summary.global_quantities.h_98 (alpha) | STRUCTURE | - | Energy confinement time enhancement factor over the IPB98(y,2) scaling | |
summary.global_quantities.h_98.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.h_98.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.global_quantities.h_mode (alpha) | STRUCTURE | H-mode flag: 0 when the plasma is in L-mode and 1 when in H-mode | ||
summary.global_quantities.h_mode.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.h_mode.value (alpha) | [summary.time] | INT_1D | Value | |
summary.global_quantities.ip (alpha) | STRUCTURE | A | Total plasma current | |
summary.global_quantities.ip.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.ip.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.global_quantities.li (alpha) | STRUCTURE | - | Internal inductance. The li_3 definition is used, i.e. li_3 = 2/R0/mu0^2/Ip^2 * int(Bp^2 dV). | |
summary.global_quantities.li.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.li.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.global_quantities.r0 (alpha) | STRUCTURE | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) | |
summary.global_quantities.r0.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.r0.value (alpha) | FLT_0D (uncertain) | m | Value | |
summary.global_quantities.resistance (alpha) | STRUCTURE | ohm | Plasma electric resistance | |
summary.global_quantities.resistance.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.resistance.value (alpha) | [summary.time] | FLT_1D (uncertain) | ohm | Value |
summary.global_quantities.tau_energy (alpha) | STRUCTURE | s | Energy confinement time | |
summary.global_quantities.tau_energy.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.tau_energy.value (alpha) | [summary.time] | FLT_1D (uncertain) | s | Value |
summary.global_quantities.tau_helium (alpha) | STRUCTURE | s | Helium confinement time | |
summary.global_quantities.tau_helium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.tau_helium.value (alpha) | [summary.time] | FLT_1D (uncertain) | s | Value |
summary.global_quantities.tau_resistive (alpha) | STRUCTURE | s | Current diffusion characteristic time | |
summary.global_quantities.tau_resistive.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.tau_resistive.value (alpha) | [summary.time] | FLT_1D (uncertain) | s | Value |
summary.global_quantities.v_loop (alpha) | STRUCTURE | V | LCFS loop voltage | |
summary.global_quantities.v_loop.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.v_loop.value (alpha) | [summary.time] | FLT_1D (uncertain) | V | Value |
summary.global_quantities.volume (alpha) | STRUCTURE | m^3 | Volume of the confined plasma | |
summary.global_quantities.volume.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.global_quantities.volume.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^3 | Value |
summary.heating_current_drive (alpha) | STRUCTURE | Heating and current drive parameters | ||
summary.heating_current_drive.ec (alpha) | [1...N] | STRUCT_ARRAY | Set of ECRH/ECCD launchers | |
summary.heating_current_drive.ec[:].angle_pol (alpha) | STRUCTURE | rad | Poloidal angle of ECRH at resonance | |
summary.heating_current_drive.ec[:].angle_pol.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ec[:].angle_pol.value (alpha) | [summary.time] | FLT_1D (uncertain) | rad | Value |
summary.heating_current_drive.ec[:].angle_tor (alpha) | STRUCTURE | rad | Toroidal angle of ECRH at resonance | |
summary.heating_current_drive.ec[:].angle_tor.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ec[:].angle_tor.value (alpha) | [summary.time] | FLT_1D (uncertain) | rad | Value |
summary.heating_current_drive.ec[:].current (alpha) | STRUCTURE | A | Parallel current driven by EC waves | |
summary.heating_current_drive.ec[:].current.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ec[:].current.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.heating_current_drive.ec[:].energy_fast (alpha) | STRUCTURE | J | Fast particle energy content driven by EC waves | |
summary.heating_current_drive.ec[:].energy_fast.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ec[:].energy_fast.value (alpha) | [summary.time] | FLT_1D (uncertain) | J | Value |
summary.heating_current_drive.ec[:].frequency (alpha) | STRUCTURE | Hz | ECRH frequency | |
summary.heating_current_drive.ec[:].frequency.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ec[:].frequency.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.heating_current_drive.ec[:].harmonic (alpha) | STRUCTURE | Harmonic number of the absorbed ECRH waves | ||
summary.heating_current_drive.ec[:].harmonic.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ec[:].harmonic.value (alpha) | [summary.time] | INT_1D | Value | |
summary.heating_current_drive.ec[:].polarisation (alpha) | STRUCTURE | Polarisation of the ECRH waves (0 = O mode, 1 = X mode) | ||
summary.heating_current_drive.ec[:].polarisation.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ec[:].polarisation.value (alpha) | [summary.time] | INT_1D | Value | |
summary.heating_current_drive.ec[:].position (alpha) | STRUCTURE | - | Position of the maximum of the ECRH power deposition, in rho_tor_norm | |
summary.heating_current_drive.ec[:].position.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ec[:].position.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.heating_current_drive.ec[:].power (alpha) | STRUCTURE | W | Electron cyclotron heating power coupled to the plasma | |
summary.heating_current_drive.ec[:].power.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ec[:].power.value (alpha) | [summary.time] | FLT_1D (uncertain) | W | Value |
summary.heating_current_drive.ic (alpha) | [1...N] | STRUCT_ARRAY | Set of ICRH launchers | |
summary.heating_current_drive.ic[:].current (alpha) | STRUCTURE | A | Parallel current driven by IC waves | |
summary.heating_current_drive.ic[:].current.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].current.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.heating_current_drive.ic[:].e_field_plus_minus_ratio (alpha) | STRUCTURE | - | Average E+/E- power ratio of IC waves | |
summary.heating_current_drive.ic[:].e_field_plus_minus_ratio.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].e_field_plus_minus_ratio.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.heating_current_drive.ic[:].energy_fast (alpha) | STRUCTURE | J | Fast particle energy content driven by IC waves | |
summary.heating_current_drive.ic[:].energy_fast.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].energy_fast.value (alpha) | [summary.time] | FLT_1D (uncertain) | J | Value |
summary.heating_current_drive.ic[:].frequency (alpha) | STRUCTURE | Hz | ICRH frequency | |
summary.heating_current_drive.ic[:].frequency.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].frequency.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.heating_current_drive.ic[:].harmonic (alpha) | STRUCTURE | Harmonic number of the absorbed ICRH waves | ||
summary.heating_current_drive.ic[:].harmonic.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].harmonic.value (alpha) | [summary.time] | INT_1D | Value | |
summary.heating_current_drive.ic[:].k_perpendicular (alpha) | STRUCTURE | m^-1 | Main perpendicular wave number of IC waves | |
summary.heating_current_drive.ic[:].k_perpendicular.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].k_perpendicular.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-1 | Value |
summary.heating_current_drive.ic[:].n_tor (alpha) | STRUCTURE | Main toroidal mode number of IC waves | ||
summary.heating_current_drive.ic[:].n_tor.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].n_tor.value (alpha) | [summary.time] | INT_1D | Value | |
summary.heating_current_drive.ic[:].phase (alpha) | STRUCTURE | rad | Phase between straps | |
summary.heating_current_drive.ic[:].phase.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].phase.value (alpha) | [summary.time] | FLT_1D (uncertain) | rad | Value |
summary.heating_current_drive.ic[:].position (alpha) | STRUCTURE | - | Position of the maximum of the ICRH power deposition, in rho_tor_norm | |
summary.heating_current_drive.ic[:].position.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].position.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.heating_current_drive.ic[:].power (alpha) | STRUCTURE | W | IC heating power coupled to the plasma | |
summary.heating_current_drive.ic[:].power.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.ic[:].power.value (alpha) | [summary.time] | FLT_1D (uncertain) | W | Value |
summary.heating_current_drive.lh (alpha) | [1...N] | STRUCT_ARRAY | Set of LHCD launchers | |
summary.heating_current_drive.lh[:].current (alpha) | STRUCTURE | A | Parallel current driven by LH waves | |
summary.heating_current_drive.lh[:].current.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.lh[:].current.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.heating_current_drive.lh[:].energy_fast (alpha) | STRUCTURE | J | Fast particle energy content driven by LH waves | |
summary.heating_current_drive.lh[:].energy_fast.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.lh[:].energy_fast.value (alpha) | [summary.time] | FLT_1D (uncertain) | J | Value |
summary.heating_current_drive.lh[:].frequency (alpha) | STRUCTURE | Hz | LH wave frequency | |
summary.heating_current_drive.lh[:].frequency.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.lh[:].frequency.value (alpha) | [summary.time] | FLT_1D (uncertain) | Hz | Value |
summary.heating_current_drive.lh[:].n_parallel (alpha) | STRUCTURE | - | Main parallel refractive index of LH waves at launch | |
summary.heating_current_drive.lh[:].n_parallel.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.lh[:].n_parallel.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.heating_current_drive.lh[:].position (alpha) | STRUCTURE | - | Position of the maximum of the LH power deposition, in rho_tor_norm | |
summary.heating_current_drive.lh[:].position.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.lh[:].position.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.heating_current_drive.lh[:].power (alpha) | STRUCTURE | W | LH heating power coupled to the plasma | |
summary.heating_current_drive.lh[:].power.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.lh[:].power.value (alpha) | [summary.time] | FLT_1D (uncertain) | W | Value |
summary.heating_current_drive.nbi (alpha) | [1...N] | STRUCT_ARRAY | Set of NBI units | |
summary.heating_current_drive.nbi[:].angle (alpha) | STRUCTURE | rad | Angle of inclination between a beamlet at the centre of the injection unit surface and the horiontal plane | |
summary.heating_current_drive.nbi[:].angle.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].angle.value (alpha) | FLT_0D (uncertain) | rad | Value | |
summary.heating_current_drive.nbi[:].beam_current_fraction (alpha) | STRUCTURE | - | Fractions of beam current distributed among the different energies, the first index corresponds to the fast neutrals energy (1:full, 2: half, 3: one third) | |
summary.heating_current_drive.nbi[:].beam_current_fraction.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].beam_current_fraction.value (alpha) | [1...3, | FLT_2D (uncertain) | - | Value |
summary.heating_current_drive.nbi[:].beam_power_fraction (alpha) | STRUCTURE | - | Fractions of beam power distributed among the different energies, the first index corresponds to the fast neutrals energy (1:full, 2: half, 3: one third) | |
summary.heating_current_drive.nbi[:].beam_power_fraction.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].beam_power_fraction.value (alpha) | [1...3, | FLT_2D (uncertain) | - | Value |
summary.heating_current_drive.nbi[:].current (alpha) | STRUCTURE | A | Parallel current driven by this NBI unit | |
summary.heating_current_drive.nbi[:].current.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].current.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.heating_current_drive.nbi[:].direction (alpha) | STRUCTURE | Direction of the beam seen from above the torus: -1 = clockwise; 1 = counter clockwise | ||
summary.heating_current_drive.nbi[:].direction.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].direction.value (alpha) | INT_0D | ? | Value | |
summary.heating_current_drive.nbi[:].energy (alpha) | STRUCTURE | eV | Full energy of the injected species (acceleration of a single atom) | |
summary.heating_current_drive.nbi[:].energy.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].energy.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.heating_current_drive.nbi[:].position (alpha) | STRUCTURE | R, Z, Phi position of the NBI unit centre | ||
summary.heating_current_drive.nbi[:].position.phi (alpha) | STRUCTURE | rad | Toroidal angle | |
summary.heating_current_drive.nbi[:].position.phi.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].position.phi.value (alpha) | FLT_0D (uncertain) | rad | Value | |
summary.heating_current_drive.nbi[:].position.r (alpha) | STRUCTURE | m | Major radius | |
summary.heating_current_drive.nbi[:].position.r.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].position.r.value (alpha) | FLT_0D (uncertain) | m | Value | |
summary.heating_current_drive.nbi[:].position.z (alpha) | STRUCTURE | m | Height | |
summary.heating_current_drive.nbi[:].position.z.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].position.z.value (alpha) | FLT_0D (uncertain) | m | Value | |
summary.heating_current_drive.nbi[:].power (alpha) | STRUCTURE | W | NBI power coupled to the plasma by this unit | |
summary.heating_current_drive.nbi[:].power.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].power.value (alpha) | [summary.time] | FLT_1D (uncertain) | W | Value |
summary.heating_current_drive.nbi[:].species (alpha) | STRUCTURE | Atomic Mass Unit | Injected species | |
summary.heating_current_drive.nbi[:].species.a (alpha) | STRUCTURE | Atomic Mass Unit | Mass of atom | |
summary.heating_current_drive.nbi[:].species.a.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].species.a.value (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Value | |
summary.heating_current_drive.nbi[:].species.label (alpha) | STRUCTURE | String identifying the species (e.g. H, D, T, ...) | ||
summary.heating_current_drive.nbi[:].species.label.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].species.label.value (alpha) | STR_0D | Value | ||
summary.heating_current_drive.nbi[:].species.z_n (alpha) | STRUCTURE | Elementary Charge Unit | Nuclear charge | |
summary.heating_current_drive.nbi[:].species.z_n.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].species.z_n.value (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Value | |
summary.heating_current_drive.nbi[:].tangency_radius (alpha) | STRUCTURE | m | Tangency radius (major radius where the central line of a NBI unit is tangent to a circle around the torus) | |
summary.heating_current_drive.nbi[:].tangency_radius.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.heating_current_drive.nbi[:].tangency_radius.value (alpha) | FLT_0D (uncertain) | m | Value | |
summary.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
summary.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
summary.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
summary.ids_properties.occurrence | INT_0D | |||
summary.line_average (alpha) | STRUCTURE | Line average plasma parameters | ||
summary.line_average.n_e (alpha) | STRUCTURE | m^-3 | Electron density | |
summary.line_average.n_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i (alpha) | STRUCTURE | m^-3 | Ion density per species | |
summary.line_average.n_i.argon (alpha) | STRUCTURE | Argon | ||
summary.line_average.n_i.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.berylium (alpha) | STRUCTURE | Berylium | ||
summary.line_average.n_i.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.carbon (alpha) | STRUCTURE | Carbon | ||
summary.line_average.n_i.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.line_average.n_i.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.line_average.n_i.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.line_average.n_i.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.line_average.n_i.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.lithium (alpha) | STRUCTURE | Lithium | ||
summary.line_average.n_i.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.neon (alpha) | STRUCTURE | Neon | ||
summary.line_average.n_i.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.line_average.n_i.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.line_average.n_i.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.tritium (alpha) | STRUCTURE | Tritium | ||
summary.line_average.n_i.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.line_average.n_i.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i.xenon (alpha) | STRUCTURE | Xenon | ||
summary.line_average.n_i.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.n_i_total (alpha) | STRUCTURE | m^-3 | Total ion density (sum over species) | |
summary.line_average.n_i_total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.n_i_total.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.line_average.t_e (alpha) | STRUCTURE | eV | Electron temperature | |
summary.line_average.t_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.t_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.line_average.t_i_average (alpha) | STRUCTURE | eV | Ion temperature (average over ion species) | |
summary.line_average.t_i_average.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.t_i_average.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.line_average.zeff (alpha) | STRUCTURE | - | Effective charge | |
summary.line_average.zeff.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.line_average.zeff.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local (alpha) | STRUCTURE | Plasma parameter values at different locations | ||
summary.local.divertor_plate (alpha) | [1...N] | STRUCT_ARRAY | Parameters at a divertor plate. RAJOUTER NAME DANS LA STRUCTURE dESSOUS | |
summary.local.divertor_plate[:].flux_expansion (alpha) | STRUCTURE | - | Flux expansion | |
summary.local.divertor_plate[:].flux_expansion.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].flux_expansion.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.divertor_plate[:].n_e (alpha) | STRUCTURE | m^-3 | Electron density | |
summary.local.divertor_plate[:].n_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i (alpha) | STRUCTURE | m^-3 | Ion density per species | |
summary.local.divertor_plate[:].n_i.argon (alpha) | STRUCTURE | Argon | ||
summary.local.divertor_plate[:].n_i.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.divertor_plate[:].n_i.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.divertor_plate[:].n_i.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.divertor_plate[:].n_i.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.divertor_plate[:].n_i.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.divertor_plate[:].n_i.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.divertor_plate[:].n_i.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.divertor_plate[:].n_i.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.neon (alpha) | STRUCTURE | Neon | ||
summary.local.divertor_plate[:].n_i.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.divertor_plate[:].n_i.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.divertor_plate[:].n_i.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.divertor_plate[:].n_i.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.divertor_plate[:].n_i.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.divertor_plate[:].n_i.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].n_i_total (alpha) | STRUCTURE | m^-3 | Total ion density (sum over species) | |
summary.local.divertor_plate[:].n_i_total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].n_i_total.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.divertor_plate[:].t_e (alpha) | STRUCTURE | eV | Electron temperature | |
summary.local.divertor_plate[:].t_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].t_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.divertor_plate[:].t_i_average (alpha) | STRUCTURE | eV | Ion temperature (average over ion species) | |
summary.local.divertor_plate[:].t_i_average.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].t_i_average.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.divertor_plate[:].zeff (alpha) | STRUCTURE | - | Effective charge | |
summary.local.divertor_plate[:].zeff.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.divertor_plate[:].zeff.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.edge (alpha) | STRUCTURE | Parameters at last closed flux surface | ||
summary.local.edge.magnetic_shear (alpha) | STRUCTURE | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor | |
summary.local.edge.magnetic_shear.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.magnetic_shear.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.edge.momentum_tor (alpha) | STRUCTURE | kg.m.s^-1 | Total plasma toroidal momentum, summed over ion species and electrons | |
summary.local.edge.momentum_tor.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.momentum_tor.value (alpha) | [summary.time] | FLT_1D (uncertain) | kg.m.s^-1 | Value |
summary.local.edge.n_e (alpha) | STRUCTURE | m^-3 | Electron density | |
summary.local.edge.n_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i (alpha) | STRUCTURE | m^-3 | Ion density per species | |
summary.local.edge.n_i.argon (alpha) | STRUCTURE | Argon | ||
summary.local.edge.n_i.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.edge.n_i.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.edge.n_i.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.edge.n_i.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.edge.n_i.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.edge.n_i.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.edge.n_i.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.edge.n_i.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.neon (alpha) | STRUCTURE | Neon | ||
summary.local.edge.n_i.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.edge.n_i.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.edge.n_i.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.edge.n_i.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.edge.n_i.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.edge.n_i.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.n_i_total (alpha) | STRUCTURE | m^-3 | Total ion density (sum over species) | |
summary.local.edge.n_i_total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.n_i_total.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.edge.position (alpha) | STRUCTURE | Radial position at which physics quantities are evaluated | ||
summary.local.edge.position.psi (alpha) | [summary.time] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
summary.local.edge.position.rho_tor (alpha) | [summary.time] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under global_quantities/b0 |
summary.local.edge.position.rho_tor_norm (alpha) | [summary.time] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
summary.local.edge.q (alpha) | STRUCTURE | - | Safety factor | |
summary.local.edge.q.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.q.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.edge.t_e (alpha) | STRUCTURE | eV | Electron temperature | |
summary.local.edge.t_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.t_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.edge.t_i_average (alpha) | STRUCTURE | eV | Ion temperature (average over ion species) | |
summary.local.edge.t_i_average.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.t_i_average.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.edge.velocity_tor (alpha) | STRUCTURE | m.s^-1 | Ion toroidal rotation velocity, per species | |
summary.local.edge.velocity_tor.argon (alpha) | STRUCTURE | Argon | ||
summary.local.edge.velocity_tor.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.edge.velocity_tor.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.edge.velocity_tor.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.edge.velocity_tor.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.edge.velocity_tor.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.edge.velocity_tor.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.edge.velocity_tor.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.edge.velocity_tor.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.neon (alpha) | STRUCTURE | Neon | ||
summary.local.edge.velocity_tor.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.edge.velocity_tor.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.edge.velocity_tor.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.edge.velocity_tor.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.edge.velocity_tor.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.velocity_tor.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.edge.velocity_tor.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.velocity_tor.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.edge.zeff (alpha) | STRUCTURE | - | Effective charge | |
summary.local.edge.zeff.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.edge.zeff.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.itb (alpha) | STRUCTURE | Parameters at internal transport barrier | ||
summary.local.itb.magnetic_shear (alpha) | STRUCTURE | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor | |
summary.local.itb.magnetic_shear.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.magnetic_shear.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.itb.momentum_tor (alpha) | STRUCTURE | kg.m.s^-1 | Total plasma toroidal momentum, summed over ion species and electrons | |
summary.local.itb.momentum_tor.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.momentum_tor.value (alpha) | [summary.time] | FLT_1D (uncertain) | kg.m.s^-1 | Value |
summary.local.itb.n_e (alpha) | STRUCTURE | m^-3 | Electron density | |
summary.local.itb.n_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i (alpha) | STRUCTURE | m^-3 | Ion density per species | |
summary.local.itb.n_i.argon (alpha) | STRUCTURE | Argon | ||
summary.local.itb.n_i.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.itb.n_i.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.itb.n_i.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.itb.n_i.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.itb.n_i.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.itb.n_i.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.itb.n_i.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.itb.n_i.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.neon (alpha) | STRUCTURE | Neon | ||
summary.local.itb.n_i.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.itb.n_i.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.itb.n_i.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.itb.n_i.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.itb.n_i.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.itb.n_i.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.n_i_total (alpha) | STRUCTURE | m^-3 | Total ion density (sum over species) | |
summary.local.itb.n_i_total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.n_i_total.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.itb.position (alpha) | STRUCTURE | Radial position at which physics quantities are evaluated | ||
summary.local.itb.position.psi (alpha) | [summary.time] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
summary.local.itb.position.rho_tor (alpha) | [summary.time] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under global_quantities/b0 |
summary.local.itb.position.rho_tor_norm (alpha) | [summary.time] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
summary.local.itb.q (alpha) | STRUCTURE | - | Safety factor | |
summary.local.itb.q.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.q.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.itb.t_e (alpha) | STRUCTURE | eV | Electron temperature | |
summary.local.itb.t_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.t_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.itb.t_i_average (alpha) | STRUCTURE | eV | Ion temperature (average over ion species) | |
summary.local.itb.t_i_average.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.t_i_average.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.itb.velocity_tor (alpha) | STRUCTURE | m.s^-1 | Ion toroidal rotation velocity, per species | |
summary.local.itb.velocity_tor.argon (alpha) | STRUCTURE | Argon | ||
summary.local.itb.velocity_tor.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.itb.velocity_tor.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.itb.velocity_tor.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.itb.velocity_tor.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.itb.velocity_tor.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.itb.velocity_tor.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.itb.velocity_tor.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.itb.velocity_tor.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.neon (alpha) | STRUCTURE | Neon | ||
summary.local.itb.velocity_tor.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.itb.velocity_tor.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.itb.velocity_tor.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.itb.velocity_tor.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.itb.velocity_tor.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.velocity_tor.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.itb.velocity_tor.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.velocity_tor.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.itb.zeff (alpha) | STRUCTURE | - | Effective charge | |
summary.local.itb.zeff.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.itb.zeff.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.limiter (alpha) | STRUCTURE | Parameters at the limiter | ||
summary.local.limiter.flux_expansion (alpha) | STRUCTURE | - | Flux expansion | |
summary.local.limiter.flux_expansion.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.flux_expansion.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.limiter.n_e (alpha) | STRUCTURE | m^-3 | Electron density | |
summary.local.limiter.n_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i (alpha) | STRUCTURE | m^-3 | Ion density per species | |
summary.local.limiter.n_i.argon (alpha) | STRUCTURE | Argon | ||
summary.local.limiter.n_i.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.limiter.n_i.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.limiter.n_i.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.limiter.n_i.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.limiter.n_i.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.limiter.n_i.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.limiter.n_i.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.limiter.n_i.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.neon (alpha) | STRUCTURE | Neon | ||
summary.local.limiter.n_i.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.limiter.n_i.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.limiter.n_i.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.limiter.n_i.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.limiter.n_i.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.limiter.n_i.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.n_i_total (alpha) | STRUCTURE | m^-3 | Total ion density (sum over species) | |
summary.local.limiter.n_i_total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.n_i_total.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.limiter.t_e (alpha) | STRUCTURE | eV | Electron temperature | |
summary.local.limiter.t_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.t_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.limiter.t_i_average (alpha) | STRUCTURE | eV | Ion temperature (average over ion species) | |
summary.local.limiter.t_i_average.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.t_i_average.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.limiter.zeff (alpha) | STRUCTURE | - | Effective charge | |
summary.local.limiter.zeff.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.limiter.zeff.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.magnetic_axis (alpha) | STRUCTURE | Parameters at magnetic axis | ||
summary.local.magnetic_axis.magnetic_shear (alpha) | STRUCTURE | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor | |
summary.local.magnetic_axis.magnetic_shear.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.magnetic_shear.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.magnetic_axis.momentum_tor (alpha) | STRUCTURE | kg.m.s^-1 | Total plasma toroidal momentum, summed over ion species and electrons | |
summary.local.magnetic_axis.momentum_tor.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.momentum_tor.value (alpha) | [summary.time] | FLT_1D (uncertain) | kg.m.s^-1 | Value |
summary.local.magnetic_axis.n_e (alpha) | STRUCTURE | m^-3 | Electron density | |
summary.local.magnetic_axis.n_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i (alpha) | STRUCTURE | m^-3 | Ion density per species | |
summary.local.magnetic_axis.n_i.argon (alpha) | STRUCTURE | Argon | ||
summary.local.magnetic_axis.n_i.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.magnetic_axis.n_i.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.magnetic_axis.n_i.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.magnetic_axis.n_i.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.magnetic_axis.n_i.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.magnetic_axis.n_i.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.magnetic_axis.n_i.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.magnetic_axis.n_i.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.neon (alpha) | STRUCTURE | Neon | ||
summary.local.magnetic_axis.n_i.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.magnetic_axis.n_i.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.magnetic_axis.n_i.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.magnetic_axis.n_i.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.magnetic_axis.n_i.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.magnetic_axis.n_i.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.n_i_total (alpha) | STRUCTURE | m^-3 | Total ion density (sum over species) | |
summary.local.magnetic_axis.n_i_total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.n_i_total.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.magnetic_axis.position (alpha) | STRUCTURE | Radial position at which physics quantities are evaluated | ||
summary.local.magnetic_axis.position.psi (alpha) | [summary.time] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
summary.local.magnetic_axis.position.r (alpha) | [summary.time] | FLT_1D (uncertain) | m | Major radius |
summary.local.magnetic_axis.position.rho_tor (alpha) | [summary.time] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under global_quantities/b0 |
summary.local.magnetic_axis.position.rho_tor_norm (alpha) | [summary.time] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
summary.local.magnetic_axis.position.z (alpha) | [summary.time] | FLT_1D (uncertain) | m | Height |
summary.local.magnetic_axis.q (alpha) | STRUCTURE | - | Safety factor | |
summary.local.magnetic_axis.q.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.q.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.magnetic_axis.t_e (alpha) | STRUCTURE | eV | Electron temperature | |
summary.local.magnetic_axis.t_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.t_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.magnetic_axis.t_i_average (alpha) | STRUCTURE | eV | Ion temperature (average over ion species) | |
summary.local.magnetic_axis.t_i_average.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.t_i_average.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.magnetic_axis.velocity_tor (alpha) | STRUCTURE | m.s^-1 | Ion toroidal rotation velocity, per species | |
summary.local.magnetic_axis.velocity_tor.argon (alpha) | STRUCTURE | Argon | ||
summary.local.magnetic_axis.velocity_tor.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.magnetic_axis.velocity_tor.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.magnetic_axis.velocity_tor.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.magnetic_axis.velocity_tor.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.magnetic_axis.velocity_tor.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.magnetic_axis.velocity_tor.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.magnetic_axis.velocity_tor.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.magnetic_axis.velocity_tor.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.neon (alpha) | STRUCTURE | Neon | ||
summary.local.magnetic_axis.velocity_tor.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.magnetic_axis.velocity_tor.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.magnetic_axis.velocity_tor.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.magnetic_axis.velocity_tor.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.magnetic_axis.velocity_tor.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.velocity_tor.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.magnetic_axis.velocity_tor.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.velocity_tor.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.magnetic_axis.zeff (alpha) | STRUCTURE | - | Effective charge | |
summary.local.magnetic_axis.zeff.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.magnetic_axis.zeff.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.pedestal (alpha) | STRUCTURE | Parameters at pedestal top | ||
summary.local.pedestal.magnetic_shear (alpha) | STRUCTURE | - | Magnetic shear, defined as rho_tor/q . dq/drho_tor | |
summary.local.pedestal.magnetic_shear.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.magnetic_shear.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.pedestal.momentum_tor (alpha) | STRUCTURE | kg.m.s^-1 | Total plasma toroidal momentum, summed over ion species and electrons | |
summary.local.pedestal.momentum_tor.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.momentum_tor.value (alpha) | [summary.time] | FLT_1D (uncertain) | kg.m.s^-1 | Value |
summary.local.pedestal.n_e (alpha) | STRUCTURE | m^-3 | Electron density | |
summary.local.pedestal.n_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i (alpha) | STRUCTURE | m^-3 | Ion density per species | |
summary.local.pedestal.n_i.argon (alpha) | STRUCTURE | Argon | ||
summary.local.pedestal.n_i.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.pedestal.n_i.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.pedestal.n_i.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.pedestal.n_i.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.pedestal.n_i.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.pedestal.n_i.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.pedestal.n_i.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.pedestal.n_i.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.neon (alpha) | STRUCTURE | Neon | ||
summary.local.pedestal.n_i.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.pedestal.n_i.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.pedestal.n_i.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.pedestal.n_i.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.pedestal.n_i.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.pedestal.n_i.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.n_i_total (alpha) | STRUCTURE | m^-3 | Total ion density (sum over species) | |
summary.local.pedestal.n_i_total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.n_i_total.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.local.pedestal.position (alpha) | STRUCTURE | Radial position at which physics quantities are evaluated | ||
summary.local.pedestal.position.psi (alpha) | [summary.time] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
summary.local.pedestal.position.rho_tor (alpha) | [summary.time] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under global_quantities/b0 |
summary.local.pedestal.position.rho_tor_norm (alpha) | [summary.time] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
summary.local.pedestal.q (alpha) | STRUCTURE | - | Safety factor | |
summary.local.pedestal.q.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.q.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.local.pedestal.t_e (alpha) | STRUCTURE | eV | Electron temperature | |
summary.local.pedestal.t_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.t_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.pedestal.t_i_average (alpha) | STRUCTURE | eV | Ion temperature (average over ion species) | |
summary.local.pedestal.t_i_average.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.t_i_average.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.local.pedestal.velocity_tor (alpha) | STRUCTURE | m.s^-1 | Ion toroidal rotation velocity, per species | |
summary.local.pedestal.velocity_tor.argon (alpha) | STRUCTURE | Argon | ||
summary.local.pedestal.velocity_tor.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.berylium (alpha) | STRUCTURE | Berylium | ||
summary.local.pedestal.velocity_tor.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.carbon (alpha) | STRUCTURE | Carbon | ||
summary.local.pedestal.velocity_tor.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.local.pedestal.velocity_tor.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.local.pedestal.velocity_tor.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.local.pedestal.velocity_tor.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.local.pedestal.velocity_tor.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.lithium (alpha) | STRUCTURE | Lithium | ||
summary.local.pedestal.velocity_tor.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.neon (alpha) | STRUCTURE | Neon | ||
summary.local.pedestal.velocity_tor.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.local.pedestal.velocity_tor.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.local.pedestal.velocity_tor.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.tritium (alpha) | STRUCTURE | Tritium | ||
summary.local.pedestal.velocity_tor.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.local.pedestal.velocity_tor.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.velocity_tor.xenon (alpha) | STRUCTURE | Xenon | ||
summary.local.pedestal.velocity_tor.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.velocity_tor.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m.s^-1 | Value |
summary.local.pedestal.zeff (alpha) | STRUCTURE | - | Effective charge | |
summary.local.pedestal.zeff.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.local.pedestal.zeff.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.runaways (alpha) | STRUCTURE | Runaway electrons | ||
summary.runaways.current (alpha) | STRUCTURE | A | Parallel current driven by the runaway electrons | |
summary.runaways.current.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.runaways.current.value (alpha) | [summary.time] | FLT_1D (uncertain) | A | Value |
summary.runaways.particles (alpha) | STRUCTURE | - | Number of runaway electrons | |
summary.runaways.particles.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.runaways.particles.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
summary.scrape_off_layer (alpha) | STRUCTURE | Scrape-Off-Layer (SOL) characteristics | ||
summary.scrape_off_layer.heat_flux_e_decay_length (alpha) | STRUCTURE | m | Electron heat flux radial decay length inv(grad qe/qe) | |
summary.scrape_off_layer.heat_flux_e_decay_length.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.scrape_off_layer.heat_flux_e_decay_length.value (alpha) | [summary.time] | FLT_1D (uncertain) | m | Value |
summary.scrape_off_layer.heat_flux_i_decay_length (alpha) | STRUCTURE | m | Ion heat flux radial decay length inv(grad qi/qi) | |
summary.scrape_off_layer.heat_flux_i_decay_length.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.scrape_off_layer.heat_flux_i_decay_length.value (alpha) | [summary.time] | FLT_1D (uncertain) | m | Value |
summary.scrape_off_layer.n_e_decay_length (alpha) | STRUCTURE | m | Electron density radial decay length inv(grad ne/ne) | |
summary.scrape_off_layer.n_e_decay_length.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.scrape_off_layer.n_e_decay_length.value (alpha) | [summary.time] | FLT_1D (uncertain) | m | Value |
summary.scrape_off_layer.n_i_total_decay_length (alpha) | STRUCTURE | m | Ion density radial decay length inv(grad ni/ni) | |
summary.scrape_off_layer.n_i_total_decay_length.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.scrape_off_layer.n_i_total_decay_length.value (alpha) | [summary.time] | FLT_1D (uncertain) | m | Value |
summary.scrape_off_layer.power_radiated (alpha) | STRUCTURE | W | Power radiated from the SOL | |
summary.scrape_off_layer.power_radiated.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.scrape_off_layer.power_radiated.value (alpha) | [summary.time] | FLT_1D (uncertain) | W | Value |
summary.scrape_off_layer.pressure_neutral (alpha) | STRUCTURE | Pa | Neutral pressure in the SOL | |
summary.scrape_off_layer.pressure_neutral.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.scrape_off_layer.pressure_neutral.value (alpha) | [summary.time] | FLT_1D (uncertain) | Pa | Value |
summary.scrape_off_layer.t_e_decay_length (alpha) | STRUCTURE | m | Electron temperature radial decay length inv(grad Te/Te) | |
summary.scrape_off_layer.t_e_decay_length.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.scrape_off_layer.t_e_decay_length.value (alpha) | [summary.time] | FLT_1D (uncertain) | m | Value |
summary.scrape_off_layer.t_i_average_decay_length (alpha) | STRUCTURE | m | Ion temperature (average over ion species) radial decay length inv(grad Ti/Ti) | |
summary.scrape_off_layer.t_i_average_decay_length.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.scrape_off_layer.t_i_average_decay_length.value (alpha) | [summary.time] | FLT_1D (uncertain) | m | Value |
summary.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
summary.volume_average (alpha) | STRUCTURE | Volume average plasma parameters | ||
summary.volume_average.n_e (alpha) | STRUCTURE | m^-3 | Electron density | |
summary.volume_average.n_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i (alpha) | STRUCTURE | m^-3 | Ion density per species | |
summary.volume_average.n_i.argon (alpha) | STRUCTURE | Argon | ||
summary.volume_average.n_i.argon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.argon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.berylium (alpha) | STRUCTURE | Berylium | ||
summary.volume_average.n_i.berylium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.berylium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.carbon (alpha) | STRUCTURE | Carbon | ||
summary.volume_average.n_i.carbon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.carbon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.deuterium (alpha) | STRUCTURE | Deuterium | ||
summary.volume_average.n_i.deuterium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.deuterium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.helium_3 (alpha) | STRUCTURE | Helium isotope with 3 nucleons | ||
summary.volume_average.n_i.helium_3.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.helium_3.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.helium_4 (alpha) | STRUCTURE | Helium isotope with 4 nucleons | ||
summary.volume_average.n_i.helium_4.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.helium_4.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.hydrogen (alpha) | STRUCTURE | Hydrogen | ||
summary.volume_average.n_i.hydrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.hydrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.lithium (alpha) | STRUCTURE | Lithium | ||
summary.volume_average.n_i.lithium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.lithium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.neon (alpha) | STRUCTURE | Neon | ||
summary.volume_average.n_i.neon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.neon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.nitrogen (alpha) | STRUCTURE | Nitrogen | ||
summary.volume_average.n_i.nitrogen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.nitrogen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.oxygen (alpha) | STRUCTURE | Oxygen | ||
summary.volume_average.n_i.oxygen.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.oxygen.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.tritium (alpha) | STRUCTURE | Tritium | ||
summary.volume_average.n_i.tritium.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.tritium.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.tungsten (alpha) | STRUCTURE | Tungsten | ||
summary.volume_average.n_i.tungsten.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.tungsten.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i.xenon (alpha) | STRUCTURE | Xenon | ||
summary.volume_average.n_i.xenon.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i.xenon.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.n_i_total (alpha) | STRUCTURE | m^-3 | Total ion density (sum over species) | |
summary.volume_average.n_i_total.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.n_i_total.value (alpha) | [summary.time] | FLT_1D (uncertain) | m^-3 | Value |
summary.volume_average.t_e (alpha) | STRUCTURE | eV | Electron temperature | |
summary.volume_average.t_e.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.t_e.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.volume_average.t_i_average (alpha) | STRUCTURE | eV | Ion temperature (average over ion species) | |
summary.volume_average.t_i_average.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.t_i_average.value (alpha) | [summary.time] | FLT_1D (uncertain) | eV | Value |
summary.volume_average.zeff (alpha) | STRUCTURE | - | Effective charge | |
summary.volume_average.zeff.source (alpha) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...) | ||
summary.volume_average.zeff.value (alpha) | [summary.time] | FLT_1D (uncertain) | - | Value |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
temporary (alpha) | Storage of undeclared data model components | |||
temporary.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
temporary.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
temporary.code.name (alpha) | STR_0D | Name of software generating IDS | ||
temporary.code.output_flag (alpha) | [temporary.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
temporary.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
temporary.code.repository (alpha) | STR_0D | URL of software repository | ||
temporary.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
temporary.constant_float0d (alpha) | [1...N] | STRUCT_ARRAY | mixed | Constant 0D float |
temporary.constant_float0d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_float0d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_float0d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_float0d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_float0d[:].value (alpha) | FLT_0D (uncertain) | - | Value | |
temporary.constant_float1d (alpha) | [1...N] | STRUCT_ARRAY | mixed | Constant 1D float |
temporary.constant_float1d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_float1d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_float1d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_float1d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_float1d[:].value (alpha) | [1...N] | FLT_1D (uncertain) | - | Value |
temporary.constant_float2d (alpha) | [1...N] | STRUCT_ARRAY | Constant 2D float | |
temporary.constant_float2d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_float2d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_float2d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_float2d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_float2d[:].value (alpha) | [1...N, | FLT_2D (uncertain) | mixed | Value |
temporary.constant_float3d (alpha) | [1...N] | STRUCT_ARRAY | Constant 3D float | |
temporary.constant_float3d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_float3d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_float3d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_float3d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_float3d[:].value (alpha) | [1...N, | FLT_3D (uncertain) | mixed | Value |
temporary.constant_float4d (alpha) | [1...N] | STRUCT_ARRAY | Constant 4D float | |
temporary.constant_float4d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_float4d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_float4d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_float4d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_float4d[:].value (alpha) | [1...N, | FLT_4D (uncertain) | mixed | Value |
temporary.constant_float5d (alpha) | [1...N] | STRUCT_ARRAY | Constant 5D float | |
temporary.constant_float5d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_float5d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_float5d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_float5d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_float5d[:].value (alpha) | [1...N, | FLT_5D (uncertain) | mixed | Value |
temporary.constant_float6d (alpha) | [1...N] | STRUCT_ARRAY | Constant 6D float | |
temporary.constant_float6d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_float6d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_float6d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_float6d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_float6d[:].value (alpha) | [1...N, | FLT_6D (uncertain) | mixed | Value |
temporary.constant_integer0d (alpha) | [1...N] | STRUCT_ARRAY | Constant 0D integer | |
temporary.constant_integer0d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_integer0d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_integer0d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_integer0d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_integer0d[:].value (alpha) | INT_0D | Value | ||
temporary.constant_integer1d (alpha) | [1...N] | STRUCT_ARRAY | Constant 1D integer | |
temporary.constant_integer1d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_integer1d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_integer1d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_integer1d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_integer1d[:].value (alpha) | [1...N] | INT_1D | Value | |
temporary.constant_integer2d (alpha) | [1...N] | STRUCT_ARRAY | Constant 2D integer | |
temporary.constant_integer2d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_integer2d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_integer2d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_integer2d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_integer2d[:].value (alpha) | [1...N, | INT_2D | mixed | Value |
temporary.constant_integer3d (alpha) | [1...N] | STRUCT_ARRAY | Constant 3D integer | |
temporary.constant_integer3d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_integer3d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_integer3d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_integer3d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_integer3d[:].value (alpha) | [1...N, | INT_3D | mixed | Value |
temporary.constant_string0d (alpha) | [1...N] | STRUCT_ARRAY | Constant 0D string | |
temporary.constant_string0d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_string0d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_string0d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_string0d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_string0d[:].value (alpha) | STR_0D | Value | ||
temporary.constant_string1d (alpha) | [1...N] | STRUCT_ARRAY | Constant 1D string | |
temporary.constant_string1d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.constant_string1d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.constant_string1d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.constant_string1d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.constant_string1d[:].value (alpha) | [1...N] | STR_1D | Value | |
temporary.dynamic_float1d (alpha) | [1...N] | STRUCT_ARRAY | Dynamic 1D float | |
temporary.dynamic_float1d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.dynamic_float1d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.dynamic_float1d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.dynamic_float1d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.dynamic_float1d[:].value (alpha) | STRUCTURE | Value | ||
temporary.dynamic_float1d[:].value.data (alpha) | [temporary.dynamic_float1d[:].value.time] | FLT_1D (uncertain) | mixed | Value |
temporary.dynamic_float1d[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
temporary.dynamic_float2d (alpha) | [1...N] | STRUCT_ARRAY | Dynamic 2D float | |
temporary.dynamic_float2d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.dynamic_float2d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.dynamic_float2d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.dynamic_float2d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.dynamic_float2d[:].value (alpha) | STRUCTURE | Value | ||
temporary.dynamic_float2d[:].value.data (alpha) | [1...N, | FLT_2D (uncertain) | mixed | Value |
temporary.dynamic_float2d[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
temporary.dynamic_float3d (alpha) | [1...N] | STRUCT_ARRAY | Dynamic 3D float | |
temporary.dynamic_float3d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.dynamic_float3d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.dynamic_float3d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.dynamic_float3d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.dynamic_float3d[:].value (alpha) | STRUCTURE | Value | ||
temporary.dynamic_float3d[:].value.data (alpha) | [1...N, | FLT_3D (uncertain) | mixed | Value |
temporary.dynamic_float3d[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
temporary.dynamic_float4d (alpha) | [1...N] | STRUCT_ARRAY | Dynamic 4D float | |
temporary.dynamic_float4d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.dynamic_float4d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.dynamic_float4d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.dynamic_float4d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.dynamic_float4d[:].value (alpha) | STRUCTURE | Value | ||
temporary.dynamic_float4d[:].value.data (alpha) | [1...N, | FLT_4D (uncertain) | mixed | Value |
temporary.dynamic_float4d[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
temporary.dynamic_float5d (alpha) | [1...N] | STRUCT_ARRAY | Dynamic 5D float | |
temporary.dynamic_float5d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.dynamic_float5d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.dynamic_float5d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.dynamic_float5d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.dynamic_float5d[:].value (alpha) | STRUCTURE | Value | ||
temporary.dynamic_float5d[:].value.data (alpha) | [1...N, | FLT_5D (uncertain) | mixed | Value |
temporary.dynamic_float5d[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
temporary.dynamic_float6d (alpha) | [1...N] | STRUCT_ARRAY | Dynamic 6D float | |
temporary.dynamic_float6d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.dynamic_float6d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.dynamic_float6d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.dynamic_float6d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.dynamic_float6d[:].value (alpha) | STRUCTURE | Value | ||
temporary.dynamic_float6d[:].value.data (alpha) | [1...N, | FLT_6D (uncertain) | mixed | Value |
temporary.dynamic_float6d[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
temporary.dynamic_integer1d (alpha) | [1...N] | STRUCT_ARRAY | Dynamic 1D integer | |
temporary.dynamic_integer1d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.dynamic_integer1d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.dynamic_integer1d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.dynamic_integer1d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.dynamic_integer1d[:].value (alpha) | STRUCTURE | Value | ||
temporary.dynamic_integer1d[:].value.data (alpha) | [temporary.dynamic_integer1d[:].value.time] | INT_1D | mixed | Value |
temporary.dynamic_integer1d[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
temporary.dynamic_integer2d (alpha) | [1...N] | STRUCT_ARRAY | Dynamic 2D integer | |
temporary.dynamic_integer2d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.dynamic_integer2d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.dynamic_integer2d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.dynamic_integer2d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.dynamic_integer2d[:].value (alpha) | STRUCTURE | Value | ||
temporary.dynamic_integer2d[:].value.data (alpha) | [1...N, | INT_2D | mixed | Value |
temporary.dynamic_integer2d[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
temporary.dynamic_integer3d (alpha) | [1...N] | STRUCT_ARRAY | Dynamic 3D integer | |
temporary.dynamic_integer3d[:].identifier (alpha) | STRUCTURE | Description of the quantity using the standard identifier structure | ||
temporary.dynamic_integer3d[:].identifier.description (alpha) | STR_0D | Verbose description | ||
temporary.dynamic_integer3d[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
temporary.dynamic_integer3d[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
temporary.dynamic_integer3d[:].value (alpha) | STRUCTURE | Value | ||
temporary.dynamic_integer3d[:].value.data (alpha) | [1...N, | INT_3D | mixed | Value |
temporary.dynamic_integer3d[:].value.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
temporary.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
temporary.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
temporary.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
temporary.ids_properties.occurrence | INT_0D | |||
temporary.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
tf (alpha) | Toroidal field coils | |||
tf.b_field_tor_vacuum_r (alpha) | STRUCTURE | Vacuum field times major radius in the toroidal field magnet. Positive sign means anti-clockwise when viewed from above | ||
tf.b_field_tor_vacuum_r.data (alpha) | [tf.b_field_tor_vacuum_r.time] | FLT_1D (uncertain) | T.m | Vacuum field times major radius in the toroidal field magnet. Positive sign means anti-clockwise when viewed from above |
tf.b_field_tor_vacuum_r.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
tf.coil (alpha) | [1...N] | STRUCT_ARRAY | Set of coils around the tokamak | |
tf.coil[:].conductor (alpha) | [1...N] | STRUCT_ARRAY | Set of conductors inside the coil. The structure can be used with size 1 for a simplified description as a single conductor. A conductor is composed of several elements, serially connected, i.e. transporting the same current. | |
tf.coil[:].conductor[:].cross_section (alpha) | STRUCTURE | The cross-section perpendicular to the TF conductor contour is described by a series of contour points, given by their relative position with respect to the start point of the first element. This cross-section is assumed constant for all elements. | ||
tf.coil[:].conductor[:].cross_section.delta_phi (alpha) | [tf.coil[:].conductor[:].cross_section.delta_r] | FLT_1D (uncertain) | rad | Toroidal angles (relative to a reference point) |
tf.coil[:].conductor[:].cross_section.delta_r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radii (relative to a reference point) |
tf.coil[:].conductor[:].cross_section.delta_z (alpha) | [tf.coil[:].conductor[:].cross_section.delta_r] | FLT_1D (uncertain) | m | Heights (relative to a reference point) |
tf.coil[:].conductor[:].current (alpha) | STRUCTURE | Current in the conductor | ||
tf.coil[:].conductor[:].current.data (alpha) | [tf.coil[:].conductor[:].current.time] | FLT_1D (uncertain) | A | Current in the conductor |
tf.coil[:].conductor[:].current.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
tf.coil[:].conductor[:].elements (alpha) | STRUCTURE | Set of geometrical elements (line segments and/or arcs of a circle) describing the contour of the TF conductor centre | ||
tf.coil[:].conductor[:].elements.centres (alpha) | STRUCTURE | Position of the centre of the arc of a circle of every element (meaningful only if type/index = 2 or 3, fill with default/empty value otherwise) | ||
tf.coil[:].conductor[:].elements.centres.phi (alpha) | [tf.coil[:].conductor[:].elements.centres.r] | FLT_1D (uncertain) | rad | Toroidal angle |
tf.coil[:].conductor[:].elements.centres.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
tf.coil[:].conductor[:].elements.centres.z (alpha) | [tf.coil[:].conductor[:].elements.centres.r] | FLT_1D (uncertain) | m | Height |
tf.coil[:].conductor[:].elements.end_points (alpha) | STRUCTURE | Position of the end point of every element. Meaningful only if type/index = 1 or 2, fill with default/empty value otherwise | ||
tf.coil[:].conductor[:].elements.end_points.phi (alpha) | [tf.coil[:].conductor[:].elements.end_points.r] | FLT_1D (uncertain) | rad | Toroidal angle |
tf.coil[:].conductor[:].elements.end_points.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
tf.coil[:].conductor[:].elements.end_points.z (alpha) | [tf.coil[:].conductor[:].elements.end_points.r] | FLT_1D (uncertain) | m | Height |
tf.coil[:].conductor[:].elements.intermediate_points (alpha) | STRUCTURE | Position of an intermediate point along the arc of circle, for every element, providing the orientation of the element (must define with the corresponding start point an aperture angle strictly inferior to PI). Meaningful only if type/index = 2, fill with default/empty value otherwise | ||
tf.coil[:].conductor[:].elements.intermediate_points.phi (alpha) | [tf.coil[:].conductor[:].elements.intermediate_points.r] | FLT_1D (uncertain) | rad | Toroidal angle |
tf.coil[:].conductor[:].elements.intermediate_points.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
tf.coil[:].conductor[:].elements.intermediate_points.z (alpha) | [tf.coil[:].conductor[:].elements.intermediate_points.r] | FLT_1D (uncertain) | m | Height |
tf.coil[:].conductor[:].elements.names (alpha) | [1...N] | STR_1D | Name or description of every element | |
tf.coil[:].conductor[:].elements.start_points (alpha) | STRUCTURE | Position of the start point of every element | ||
tf.coil[:].conductor[:].elements.start_points.phi (alpha) | [tf.coil[:].conductor[:].elements.start_points.r] | FLT_1D (uncertain) | rad | Toroidal angle |
tf.coil[:].conductor[:].elements.start_points.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
tf.coil[:].conductor[:].elements.start_points.z (alpha) | [tf.coil[:].conductor[:].elements.start_points.r] | FLT_1D (uncertain) | m | Height |
tf.coil[:].conductor[:].elements.types (alpha) | [tf.coil[:].conductor[:].elements.names] | INT_1D | Type of every element: 1: line segment, its ends are given by the start and end points; index = 2: arc of a circle; index = 3: full circle | |
tf.coil[:].conductor[:].resistance (alpha) | FLT_0D (uncertain) | Ohm | conductor resistance | |
tf.coil[:].conductor[:].voltage (alpha) | STRUCTURE | Voltage on the conductor terminals | ||
tf.coil[:].conductor[:].voltage.data (alpha) | [tf.coil[:].conductor[:].voltage.time] | FLT_1D (uncertain) | V | Voltage on the conductor terminals |
tf.coil[:].conductor[:].voltage.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
tf.coil[:].current (alpha) | STRUCTURE | Current in the coil | ||
tf.coil[:].current.data (alpha) | [tf.coil[:].current.time] | FLT_1D (uncertain) | A | Current in the coil |
tf.coil[:].current.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
tf.coil[:].resistance (alpha) | FLT_0D (uncertain) | Ohm | Coil resistance | |
tf.coil[:].turns (alpha) | FLT_0D (uncertain) | - | Number of total turns in a toroidal field coil. May be a fraction when describing the coil connections. | |
tf.coil[:].voltage (alpha) | STRUCTURE | Voltage on the coil terminals | ||
tf.coil[:].voltage.data (alpha) | [tf.coil[:].voltage.time] | FLT_1D (uncertain) | V | Voltage on the coil terminals |
tf.coil[:].voltage.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
tf.coils_n (alpha) | INT_0D | Number of coils around the torus, in case is_periodic = 1 | ||
tf.field_map (alpha) | [tf.field_map[:].time] | STRUCT_ARRAY | Map of the vacuum field at various time slices, represented using the generic grid description | |
tf.field_map[:].a_field_r (alpha) | [1...N] | STRUCT_ARRAY | T.m | R component of the vacuum vector potential, given on various grid subsets |
tf.field_map[:].a_field_r[:].coefficients (alpha) | [tf.field_map[:].a_field_r[:].values, | FLT_2D (uncertain) | T.m | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
tf.field_map[:].a_field_r[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
tf.field_map[:].a_field_r[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
tf.field_map[:].a_field_r[:].values (alpha) | [1...N] | FLT_1D (uncertain) | T.m | One scalar value is provided per element in the grid subset. |
tf.field_map[:].a_field_tor (alpha) | [1...N] | STRUCT_ARRAY | T.m | Toroidal component of the vacuum vector potential, given on various grid subsets |
tf.field_map[:].a_field_tor[:].coefficients (alpha) | [tf.field_map[:].a_field_tor[:].values, | FLT_2D (uncertain) | T.m | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
tf.field_map[:].a_field_tor[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
tf.field_map[:].a_field_tor[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
tf.field_map[:].a_field_tor[:].values (alpha) | [1...N] | FLT_1D (uncertain) | T.m | One scalar value is provided per element in the grid subset. |
tf.field_map[:].a_field_z (alpha) | [1...N] | STRUCT_ARRAY | T.m | Z component of the vacuum vector potential, given on various grid subsets |
tf.field_map[:].a_field_z[:].coefficients (alpha) | [tf.field_map[:].a_field_z[:].values, | FLT_2D (uncertain) | T.m | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
tf.field_map[:].a_field_z[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
tf.field_map[:].a_field_z[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
tf.field_map[:].a_field_z[:].values (alpha) | [1...N] | FLT_1D (uncertain) | T.m | One scalar value is provided per element in the grid subset. |
tf.field_map[:].b_field_r (alpha) | [1...N] | STRUCT_ARRAY | T | R component of the vacuum magnetic field, given on various grid subsets |
tf.field_map[:].b_field_r[:].coefficients (alpha) | [tf.field_map[:].b_field_r[:].values, | FLT_2D (uncertain) | T | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
tf.field_map[:].b_field_r[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
tf.field_map[:].b_field_r[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
tf.field_map[:].b_field_r[:].values (alpha) | [1...N] | FLT_1D (uncertain) | T | One scalar value is provided per element in the grid subset. |
tf.field_map[:].b_field_tor (alpha) | [1...N] | STRUCT_ARRAY | T | Toroidal component of the vacuum magnetic field, given on various grid subsets |
tf.field_map[:].b_field_tor[:].coefficients (alpha) | [tf.field_map[:].b_field_tor[:].values, | FLT_2D (uncertain) | T | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
tf.field_map[:].b_field_tor[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
tf.field_map[:].b_field_tor[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
tf.field_map[:].b_field_tor[:].values (alpha) | [1...N] | FLT_1D (uncertain) | T | One scalar value is provided per element in the grid subset. |
tf.field_map[:].b_field_z (alpha) | [1...N] | STRUCT_ARRAY | T | Z component of the vacuum magnetic field, given on various grid subsets |
tf.field_map[:].b_field_z[:].coefficients (alpha) | [tf.field_map[:].b_field_z[:].values, | FLT_2D (uncertain) | T | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
tf.field_map[:].b_field_z[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
tf.field_map[:].b_field_z[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
tf.field_map[:].b_field_z[:].values (alpha) | [1...N] | FLT_1D (uncertain) | T | One scalar value is provided per element in the grid subset. |
tf.field_map[:].grid (alpha) | STRUCTURE | Grid description | ||
tf.field_map[:].grid.grid_subset (alpha) | [1...N] | STRUCT_ARRAY | Grid subsets | |
tf.field_map[:].grid.grid_subset[:].base (alpha) | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
tf.field_map[:].grid.grid_subset[:].base[:].jacobian (alpha) | [tf.field_map[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
tf.field_map[:].grid.grid_subset[:].base[:].tensor_contravariant (alpha) | [tf.field_map[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
tf.field_map[:].grid.grid_subset[:].base[:].tensor_covariant (alpha) | [tf.field_map[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
tf.field_map[:].grid.grid_subset[:].dimension (alpha) | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
tf.field_map[:].grid.grid_subset[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
tf.field_map[:].grid.grid_subset[:].element[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
tf.field_map[:].grid.grid_subset[:].element[:].object[:].dimension (alpha) | INT_0D | Dimension of the object | ||
tf.field_map[:].grid.grid_subset[:].element[:].object[:].index (alpha) | INT_0D | Object index | ||
tf.field_map[:].grid.grid_subset[:].element[:].object[:].space (alpha) | INT_0D | Index of the space from which that object is taken | ||
tf.field_map[:].grid.grid_subset[:].identifier (alpha) | STRUCTURE | Grid subset identifier | ||
tf.field_map[:].grid.grid_subset[:].identifier.description (alpha) | STR_0D | Verbose description | ||
tf.field_map[:].grid.grid_subset[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
tf.field_map[:].grid.grid_subset[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
tf.field_map[:].grid.grid_subset[:].metric (alpha) | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
tf.field_map[:].grid.grid_subset[:].metric.jacobian (alpha) | [tf.field_map[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
tf.field_map[:].grid.grid_subset[:].metric.tensor_contravariant (alpha) | [tf.field_map[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
tf.field_map[:].grid.grid_subset[:].metric.tensor_covariant (alpha) | [tf.field_map[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
tf.field_map[:].grid.identifier (alpha) | STRUCTURE | Grid identifier | ||
tf.field_map[:].grid.identifier.description (alpha) | STR_0D | Verbose description | ||
tf.field_map[:].grid.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
tf.field_map[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
tf.field_map[:].grid.space (alpha) | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
tf.field_map[:].grid.space[:].coordinates_type (alpha) | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therfore defines the dimension of the space. The meaning of these predefined integer constants can be found in the documentation of the grid service library | |
tf.field_map[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier) | ||
tf.field_map[:].grid.space[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
tf.field_map[:].grid.space[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
tf.field_map[:].grid.space[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
tf.field_map[:].grid.space[:].objects_per_dimension (alpha) | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
tf.field_map[:].grid.space[:].objects_per_dimension[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
tf.field_map[:].grid.space[:].objects_per_dimension[:].object[:].boundary (alpha) | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
tf.field_map[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].index (alpha) | INT_0D | Index of this (n-1)-dimensional boundary object | ||
tf.field_map[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].neighbours (alpha) | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
tf.field_map[:].grid.space[:].objects_per_dimension[:].object[:].geometry (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. |
tf.field_map[:].grid.space[:].objects_per_dimension[:].object[:].measure (alpha) | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
tf.field_map[:].grid.space[:].objects_per_dimension[:].object[:].nodes (alpha) | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
tf.field_map[:].time (alpha) | FLT_0D | s | Time | |
tf.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
tf.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
tf.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
tf.ids_properties.occurrence | INT_0D | |||
tf.is_periodic (alpha) | INT_0D | Flag indicating whether coils are described one by one in the coil() structure (flag=0) or whether the coil structure represents only coils having different characteristics (flag = 1, n_coils must be filled in that case). In the latter case, the coil() sequence is repeated periodically around the torus. | ||
tf.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
thomson_scattering (alpha) | Thomson scattering diagnostic | |||
thomson_scattering.channel (alpha) | [1...N] | STRUCT_ARRAY | Set of channels (lines-of-sight) | |
thomson_scattering.channel[:].identifier (alpha) | STR_0D | ID of the channel | ||
thomson_scattering.channel[:].n_e (alpha) | STRUCTURE | Electron density | ||
thomson_scattering.channel[:].n_e.data (alpha) | [thomson_scattering.channel[:].n_e.time] | FLT_1D (uncertain) | m^-3 | Electron density |
thomson_scattering.channel[:].n_e.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
thomson_scattering.channel[:].name (alpha) | STR_0D | Name of the channel | ||
thomson_scattering.channel[:].position (alpha) | STRUCTURE | Position of the measurements (intersection between laser beam and line of sight) | ||
thomson_scattering.channel[:].position.phi (alpha) | FLT_0D (uncertain) | rad | Toroidal angle | |
thomson_scattering.channel[:].position.r (alpha) | FLT_0D (uncertain) | m | Major radius | |
thomson_scattering.channel[:].position.z (alpha) | FLT_0D (uncertain) | m | Height | |
thomson_scattering.channel[:].t_e (alpha) | STRUCTURE | Electron temperature | ||
thomson_scattering.channel[:].t_e.data (alpha) | [thomson_scattering.channel[:].t_e.time] | FLT_1D (uncertain) | eV | Electron temperature |
thomson_scattering.channel[:].t_e.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
thomson_scattering.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
thomson_scattering.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
thomson_scattering.code.name (alpha) | STR_0D | Name of software generating IDS | ||
thomson_scattering.code.output_flag (alpha) | [thomson_scattering.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
thomson_scattering.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
thomson_scattering.code.repository (alpha) | STR_0D | URL of software repository | ||
thomson_scattering.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
thomson_scattering.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
thomson_scattering.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
thomson_scattering.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
thomson_scattering.ids_properties.occurrence | INT_0D | |||
thomson_scattering.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
transport_solver_numerics (alpha) | Numerical quantities used by transport solvers and convergence details | |||
transport_solver_numerics.boundary_conditions_1d (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].time] | STRUCT_ARRAY | Boundary conditions of the radial transport equations for various time slices. To be removed when the profiles_1d structure is finalized. | |
transport_solver_numerics.boundary_conditions_1d[:].current (alpha) | STRUCTURE | Boundary condition for the current diffusion equation. | ||
transport_solver_numerics.boundary_conditions_1d[:].current.identifier (alpha) | [transport_solver_numerics.grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: poloidal flux; 2: ip; 3: loop voltage; 4: undefined; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.boundary_conditions_1d[:].current.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].current.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].current.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].current.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.boundary_conditions_1d[:].current.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 3, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.boundary_conditions_1d[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
transport_solver_numerics.boundary_conditions_1d[:].electrons.energy (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Boundary condition for the electron energy equation (temperature if ID = 1) |
transport_solver_numerics.boundary_conditions_1d[:].electrons.energy.identifier (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.boundary_conditions_1d[:].electrons.energy.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].electrons.energy.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].electrons.energy.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].electrons.energy.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.boundary_conditions_1d[:].electrons.energy.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.boundary_conditions_1d[:].electrons.particles (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Boundary condition for the electron density equation (density if ID = 1) |
transport_solver_numerics.boundary_conditions_1d[:].electrons.particles.identifier (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.boundary_conditions_1d[:].electrons.particles.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].electrons.particles.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].electrons.particles.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].electrons.particles.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.boundary_conditions_1d[:].electrons.particles.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.boundary_conditions_1d[:].energy_ion_total (alpha) | [transport_solver_numerics.grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Boundary condition for the ion total (sum over ion species) energy equation (temperature if ID = 1) |
transport_solver_numerics.boundary_conditions_1d[:].energy_ion_total.identifier (alpha) | [transport_solver_numerics.grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.boundary_conditions_1d[:].energy_ion_total.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].energy_ion_total.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].energy_ion_total.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].energy_ion_total.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.boundary_conditions_1d[:].energy_ion_total.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.boundary_conditions_1d[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].energy (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Boundary condition for the ion energy equation (temperature if ID = 1) |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].energy.identifier (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].energy.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].energy.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].energy.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].energy.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].energy.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].particles (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Boundary condition for the ion density equation (density if ID = 1) |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].particles.identifier (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].particles.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].particles.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].particles.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].particles.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].particles.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].energy (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].ion[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Boundary condition for the charge state energy equation (temperature if ID = 1) |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].energy.identifier (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].ion[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].energy.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].energy.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].energy.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].energy.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].energy.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].is_neutral (alpha) | INT_0D | Flag specifying if this state corresponds to a neutral (1) or not (0) | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].neutral_type (alpha) | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].neutral_type.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].neutral_type.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].particles (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].ion[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Boundary condition for the charge state density equation (density if ID = 1) |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].particles.identifier (alpha) | [transport_solver_numerics.boundary_conditions_1d[:].ion[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].particles.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].particles.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].particles.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].particles.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].particles.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
transport_solver_numerics.boundary_conditions_1d[:].ion[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
transport_solver_numerics.boundary_conditions_1d[:].momentum_tor (alpha) | [transport_solver_numerics.grid.rho_tor_norm] | STRUCTURE | kg.m.s^-1 | Boundary condition for the total plasma toroidal momentum equation (summed over ion species and electrons) (momentum if ID = 1) |
transport_solver_numerics.boundary_conditions_1d[:].momentum_tor.identifier (alpha) | [transport_solver_numerics.grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.boundary_conditions_1d[:].momentum_tor.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_1d[:].momentum_tor.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_1d[:].momentum_tor.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_1d[:].momentum_tor.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.boundary_conditions_1d[:].momentum_tor.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.boundary_conditions_1d[:].time (alpha) | FLT_0D | s | Time | |
transport_solver_numerics.boundary_conditions_ggd (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].time] | STRUCT_ARRAY | Boundary conditions of the transport equations, provided on the GGD, for various time slices | |
transport_solver_numerics.boundary_conditions_ggd[:].current (alpha) | [1...N] | STRUCT_ARRAY | Boundary condition for the current diffusion equation, on various grid subsets | |
transport_solver_numerics.boundary_conditions_ggd[:].current[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
transport_solver_numerics.boundary_conditions_ggd[:].current[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
transport_solver_numerics.boundary_conditions_ggd[:].current[:].identifier (alpha) | [transport_solver_numerics.grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. List of options TBD. |
transport_solver_numerics.boundary_conditions_ggd[:].current[:].identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].current[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].current[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].current[:].values (alpha) | [1...N, | FLT_2D (uncertain) | mixed | List of vector components, one list per element in the grid subset. First dimenstion: element index. Second dimension: vector component index (for ID = 1 to 3, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3) |
transport_solver_numerics.boundary_conditions_ggd[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.energy (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Boundary condition for the electron energy equation (temperature if ID = 1), on various grid subsets |
transport_solver_numerics.boundary_conditions_ggd[:].electrons.energy[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.energy[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.energy[:].identifier (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. List of options TBD. |
transport_solver_numerics.boundary_conditions_ggd[:].electrons.energy[:].identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.energy[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.energy[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.energy[:].values (alpha) | [1...N, | FLT_2D (uncertain) | mixed | List of vector components, one list per element in the grid subset. First dimenstion: element index. Second dimension: vector component index (for ID = 1 to 3, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3) |
transport_solver_numerics.boundary_conditions_ggd[:].electrons.particles (alpha) | [1...N] | STRUCT_ARRAY | m^-3.s^-1 | Boundary condition for the electron density equation (density if ID = 1), on various grid subsets |
transport_solver_numerics.boundary_conditions_ggd[:].electrons.particles[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.particles[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.particles[:].identifier (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. List of options TBD. |
transport_solver_numerics.boundary_conditions_ggd[:].electrons.particles[:].identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.particles[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.particles[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].electrons.particles[:].values (alpha) | [1...N, | FLT_2D (uncertain) | mixed | List of vector components, one list per element in the grid subset. First dimenstion: element index. Second dimension: vector component index (for ID = 1 to 3, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3) |
transport_solver_numerics.boundary_conditions_ggd[:].grid (alpha) | STRUCTURE | Grid description | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset (alpha) | [1...N] | STRUCT_ARRAY | Grid subsets | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].base (alpha) | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].base[:].jacobian (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].base[:].tensor_contravariant (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].base[:].tensor_covariant (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].dimension (alpha) | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element[:].object[:].dimension (alpha) | INT_0D | Dimension of the object | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element[:].object[:].index (alpha) | INT_0D | Object index | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element[:].object[:].space (alpha) | INT_0D | Index of the space from which that object is taken | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].identifier (alpha) | STRUCTURE | Grid subset identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].metric (alpha) | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].metric.jacobian (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].metric.tensor_contravariant (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].metric.tensor_covariant (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
transport_solver_numerics.boundary_conditions_ggd[:].grid.identifier (alpha) | STRUCTURE | Grid identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space (alpha) | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].coordinates_type (alpha) | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therfore defines the dimension of the space. The meaning of these predefined integer constants can be found in the documentation of the grid service library | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier) | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension (alpha) | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary (alpha) | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].index (alpha) | INT_0D | Index of this (n-1)-dimensional boundary object | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].neighbours (alpha) | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].object[:].geometry (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].object[:].measure (alpha) | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].object[:].nodes (alpha) | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
transport_solver_numerics.boundary_conditions_ggd[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].energy (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Boundary condition for the ion energy equation (temperature if ID = 1), on various grid subsets |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].energy[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].energy[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].energy[:].identifier (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. List of options TBD. |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].energy[:].identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].energy[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].energy[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].energy[:].values (alpha) | [1...N, | FLT_2D (uncertain) | mixed | List of vector components, one list per element in the grid subset. First dimenstion: element index. Second dimension: vector component index (for ID = 1 to 3, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3) |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].particles (alpha) | [1...N] | STRUCT_ARRAY | m^-3.s^-1 | Boundary condition for the ion density equation (density if ID = 1), on various grid subsets |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].particles[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].particles[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].particles[:].identifier (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. List of options TBD. |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].particles[:].identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].particles[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].particles[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].particles[:].values (alpha) | [1...N, | FLT_2D (uncertain) | mixed | List of vector components, one list per element in the grid subset. First dimenstion: element index. Second dimension: vector component index (for ID = 1 to 3, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3) |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].energy (alpha) | [1...N] | STRUCT_ARRAY | W.m^-3 | Boundary condition for the charge state energy equation (temperature if ID = 1), on various grid subsets |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].energy[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].energy[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].energy[:].identifier (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].ion[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. List of options TBD. |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].energy[:].identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].energy[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].energy[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].energy[:].values (alpha) | [1...N, | FLT_2D (uncertain) | mixed | List of vector components, one list per element in the grid subset. First dimenstion: element index. Second dimension: vector component index (for ID = 1 to 3, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3) |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].is_neutral (alpha) | INT_0D | Flag specifying if this state corresponds to a neutral (1) or not (0) | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].neutral_type (alpha) | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].neutral_type.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].neutral_type.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].particles (alpha) | [1...N] | STRUCT_ARRAY | m^-3.s^-1 | Boundary condition for the charge state density equation (density if ID = 1), on various grid subsets |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].particles[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].particles[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].particles[:].identifier (alpha) | [transport_solver_numerics.boundary_conditions_ggd[:].ion[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. List of options TBD. |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].particles[:].identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].particles[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].particles[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].particles[:].values (alpha) | [1...N, | FLT_2D (uncertain) | mixed | List of vector components, one list per element in the grid subset. First dimenstion: element index. Second dimension: vector component index (for ID = 1 to 3, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3) |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle | |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
transport_solver_numerics.boundary_conditions_ggd[:].ion[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
transport_solver_numerics.boundary_conditions_ggd[:].time (alpha) | FLT_0D | s | Time | |
transport_solver_numerics.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
transport_solver_numerics.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
transport_solver_numerics.code.name (alpha) | STR_0D | Name of software generating IDS | ||
transport_solver_numerics.code.output_flag (alpha) | [transport_solver_numerics.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
transport_solver_numerics.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
transport_solver_numerics.code.repository (alpha) | STR_0D | URL of software repository | ||
transport_solver_numerics.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
transport_solver_numerics.convergence (alpha) | STRUCTURE | Convergence details | ||
transport_solver_numerics.convergence.equations (alpha) | [transport_solver_numerics.convergence.equations[:].time] | STRUCT_ARRAY | Convergence details of the transport equations, for various time slices | |
transport_solver_numerics.convergence.equations[:].current (alpha) | STRUCTURE | Convergence details of the current diffusion equation | ||
transport_solver_numerics.convergence.equations[:].current.iterations_n (alpha) | INT_0D | Number of iterations carried out in the convergence loop | ||
transport_solver_numerics.convergence.equations[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
transport_solver_numerics.convergence.equations[:].electrons.energy (alpha) | [transport_solver_numerics.convergence.equations[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Convergence details of the electron energy equation |
transport_solver_numerics.convergence.equations[:].electrons.energy.iterations_n (alpha) | INT_0D | Number of iterations carried out in the convergence loop | ||
transport_solver_numerics.convergence.equations[:].electrons.particles (alpha) | [transport_solver_numerics.convergence.equations[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Convergence details of the electron density equation |
transport_solver_numerics.convergence.equations[:].electrons.particles.iterations_n (alpha) | INT_0D | Number of iterations carried out in the convergence loop | ||
transport_solver_numerics.convergence.equations[:].energy_ion_total (alpha) | [transport_solver_numerics.convergence.grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Convergence details of the ion total (sum over ion species) energy equation |
transport_solver_numerics.convergence.equations[:].energy_ion_total.iterations_n (alpha) | INT_0D | Number of iterations carried out in the convergence loop | ||
transport_solver_numerics.convergence.equations[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
transport_solver_numerics.convergence.equations[:].ion[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
transport_solver_numerics.convergence.equations[:].ion[:].energy (alpha) | [transport_solver_numerics.convergence.equations[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Convergence details of the ion energy equation |
transport_solver_numerics.convergence.equations[:].ion[:].energy.iterations_n (alpha) | INT_0D | Number of iterations carried out in the convergence loop | ||
transport_solver_numerics.convergence.equations[:].ion[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
transport_solver_numerics.convergence.equations[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
transport_solver_numerics.convergence.equations[:].ion[:].particles (alpha) | [transport_solver_numerics.convergence.equations[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Convergence details of the ion density equation |
transport_solver_numerics.convergence.equations[:].ion[:].particles.iterations_n (alpha) | INT_0D | Number of iterations carried out in the convergence loop | ||
transport_solver_numerics.convergence.equations[:].ion[:].state (alpha) | [1...N] | STRUCT_ARRAY | Convergence details of the related to the different states transport equations | |
transport_solver_numerics.convergence.equations[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].energy (alpha) | [transport_solver_numerics.convergence.equations[:].ion[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Convergence details of the charge state energy equation |
transport_solver_numerics.convergence.equations[:].ion[:].state[:].energy.iterations_n (alpha) | INT_0D | Number of iterations carried out in the convergence loop | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].is_neutral (alpha) | INT_0D | Flag specifying if this state corresponds to a neutral (1) or not (0) | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].neutral_type (alpha) | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].neutral_type.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].neutral_type.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].particles (alpha) | [transport_solver_numerics.convergence.equations[:].ion[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Convergence details of the charge state density equation |
transport_solver_numerics.convergence.equations[:].ion[:].state[:].particles.iterations_n (alpha) | INT_0D | Number of iterations carried out in the convergence loop | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
transport_solver_numerics.convergence.equations[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle | |
transport_solver_numerics.convergence.equations[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
transport_solver_numerics.convergence.equations[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
transport_solver_numerics.convergence.equations[:].ion[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
transport_solver_numerics.convergence.equations[:].time (alpha) | FLT_0D | s | Time | |
transport_solver_numerics.convergence.time_step (alpha) | STRUCTURE | Internal time step used by the transport solver (assuming all transport equations are solved with the same time step) | ||
transport_solver_numerics.convergence.time_step.data (alpha) | [transport_solver_numerics.convergence.time_step.time] | FLT_1D (uncertain) | s | Internal time step used by the transport solver (assuming all transport equations are solved with the same time step) |
transport_solver_numerics.convergence.time_step.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
transport_solver_numerics.derivatives_1d (alpha) | [transport_solver_numerics.derivatives_1d[:].time] | STRUCT_ARRAY | Radial profiles derivatives for various time slices. To be removed when the profiles_1d structure is finalized. | |
transport_solver_numerics.derivatives_1d[:].d2_drho_tor_norm2 (alpha) | STRUCTURE | Second derivatives of total ion quantities with respect to the normalised toroidal flux | ||
transport_solver_numerics.derivatives_1d[:].d2_drho_tor_norm2.n_i_total_over_n_e (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal) |
transport_solver_numerics.derivatives_1d[:].d2_drho_tor_norm2.pressure_ion_total (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total thermal ion pressure |
transport_solver_numerics.derivatives_1d[:].d2psi_drho_tor2 (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb.m^-2 | Second derivative of the poloidal flux profile with respect to the toroidal flux coordinate |
transport_solver_numerics.derivatives_1d[:].d_drho_tor_norm (alpha) | STRUCTURE | Derivatives of total ion quantities with respect to the normalised toroidal flux | ||
transport_solver_numerics.derivatives_1d[:].d_drho_tor_norm.n_i_total_over_n_e (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal) |
transport_solver_numerics.derivatives_1d[:].d_drho_tor_norm.pressure_ion_total (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total thermal ion pressure |
transport_solver_numerics.derivatives_1d[:].d_dt (alpha) | STRUCTURE | Derivatives of total ion quantities with respect to time | ||
transport_solver_numerics.derivatives_1d[:].d_dt.n_i_total_over_n_e (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal) |
transport_solver_numerics.derivatives_1d[:].d_dt.pressure_ion_total (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Total thermal ion pressure |
transport_solver_numerics.derivatives_1d[:].d_dvolume_drho_tor_dt (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Partial derivative with respect to time of the derivative of the volume with respect to the toroidal flux coordinate |
transport_solver_numerics.derivatives_1d[:].dpsi_drho_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb.m^-1 | Derivative of the poloidal flux profile with respect to the toroidal flux coordinate |
transport_solver_numerics.derivatives_1d[:].dpsi_dt (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V | Derivative of the poloidal flux profile with respect to time |
transport_solver_numerics.derivatives_1d[:].dpsi_dt_cphi (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V | Derivative of the poloidal flux profile with respect to time, at constant toroidal flux |
transport_solver_numerics.derivatives_1d[:].dpsi_dt_crho_tor_norm (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V | Derivative of the poloidal flux profile with respect to time, at constant normalised toroidal flux coordinate |
transport_solver_numerics.derivatives_1d[:].drho_tor_dt (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Partial derivative of the toroidal flux coordinate profile with respect to time |
transport_solver_numerics.derivatives_1d[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
transport_solver_numerics.derivatives_1d[:].electrons.d2_drho_tor_norm2 (alpha) | STRUCTURE | Second derivatives with respect to the normalised toroidal flux | ||
transport_solver_numerics.derivatives_1d[:].electrons.d2_drho_tor_norm2.density (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
transport_solver_numerics.derivatives_1d[:].electrons.d2_drho_tor_norm2.density_fast (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
transport_solver_numerics.derivatives_1d[:].electrons.d2_drho_tor_norm2.pressure (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure |
transport_solver_numerics.derivatives_1d[:].electrons.d2_drho_tor_norm2.pressure_fast_parallel (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
transport_solver_numerics.derivatives_1d[:].electrons.d2_drho_tor_norm2.pressure_fast_perpendicular (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
transport_solver_numerics.derivatives_1d[:].electrons.d2_drho_tor_norm2.temperature (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
transport_solver_numerics.derivatives_1d[:].electrons.d2_drho_tor_norm2.velocity_pol (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
transport_solver_numerics.derivatives_1d[:].electrons.d2_drho_tor_norm2.velocity_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
transport_solver_numerics.derivatives_1d[:].electrons.d_drho_tor_norm (alpha) | STRUCTURE | Derivatives with respect to the normalised toroidal flux | ||
transport_solver_numerics.derivatives_1d[:].electrons.d_drho_tor_norm.density (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
transport_solver_numerics.derivatives_1d[:].electrons.d_drho_tor_norm.density_fast (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
transport_solver_numerics.derivatives_1d[:].electrons.d_drho_tor_norm.pressure (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure |
transport_solver_numerics.derivatives_1d[:].electrons.d_drho_tor_norm.pressure_fast_parallel (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
transport_solver_numerics.derivatives_1d[:].electrons.d_drho_tor_norm.pressure_fast_perpendicular (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
transport_solver_numerics.derivatives_1d[:].electrons.d_drho_tor_norm.temperature (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
transport_solver_numerics.derivatives_1d[:].electrons.d_drho_tor_norm.velocity_pol (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
transport_solver_numerics.derivatives_1d[:].electrons.d_drho_tor_norm.velocity_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
transport_solver_numerics.derivatives_1d[:].electrons.d_dt (alpha) | STRUCTURE | Derivatives with respect to time | ||
transport_solver_numerics.derivatives_1d[:].electrons.d_dt.density (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
transport_solver_numerics.derivatives_1d[:].electrons.d_dt.density_fast (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
transport_solver_numerics.derivatives_1d[:].electrons.d_dt.pressure (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure |
transport_solver_numerics.derivatives_1d[:].electrons.d_dt.pressure_fast_parallel (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
transport_solver_numerics.derivatives_1d[:].electrons.d_dt.pressure_fast_perpendicular (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
transport_solver_numerics.derivatives_1d[:].electrons.d_dt.temperature (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
transport_solver_numerics.derivatives_1d[:].electrons.d_dt.velocity_pol (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
transport_solver_numerics.derivatives_1d[:].electrons.d_dt.velocity_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
transport_solver_numerics.derivatives_1d[:].grid (alpha) | STRUCTURE | Radial grid | ||
transport_solver_numerics.derivatives_1d[:].grid.area (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
transport_solver_numerics.derivatives_1d[:].grid.psi (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
transport_solver_numerics.derivatives_1d[:].grid.rho_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm (alpha) | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
transport_solver_numerics.derivatives_1d[:].grid.volume (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
transport_solver_numerics.derivatives_1d[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
transport_solver_numerics.derivatives_1d[:].ion[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
transport_solver_numerics.derivatives_1d[:].ion[:].d2_drho_tor_norm2 (alpha) | STRUCTURE | Second derivatives with respect to the normalised toroidal flux | ||
transport_solver_numerics.derivatives_1d[:].ion[:].d2_drho_tor_norm2.density (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d2_drho_tor_norm2.density_fast (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d2_drho_tor_norm2.pressure (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d2_drho_tor_norm2.pressure_fast_parallel (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d2_drho_tor_norm2.pressure_fast_perpendicular (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d2_drho_tor_norm2.temperature (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d2_drho_tor_norm2.velocity_pol (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d2_drho_tor_norm2.velocity_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_drho_tor_norm (alpha) | STRUCTURE | Derivatives with respect to the normalised toroidal flux | ||
transport_solver_numerics.derivatives_1d[:].ion[:].d_drho_tor_norm.density (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_drho_tor_norm.density_fast (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_drho_tor_norm.pressure (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_drho_tor_norm.pressure_fast_parallel (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_drho_tor_norm.pressure_fast_perpendicular (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_drho_tor_norm.temperature (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_drho_tor_norm.velocity_pol (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_drho_tor_norm.velocity_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_dt (alpha) | STRUCTURE | Derivatives with respect to time | ||
transport_solver_numerics.derivatives_1d[:].ion[:].d_dt.density (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_dt.density_fast (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_dt.pressure (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_dt.pressure_fast_parallel (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_dt.pressure_fast_perpendicular (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_dt.temperature (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_dt.velocity_pol (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].d_dt.velocity_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity (average over charge states when multiple charge states are considered) |
transport_solver_numerics.derivatives_1d[:].ion[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
transport_solver_numerics.derivatives_1d[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d2_drho_tor_norm2 (alpha) | STRUCTURE | Second derivatives with respect to the normalised toroidal flux | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d2_drho_tor_norm2.density (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d2_drho_tor_norm2.density_fast (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d2_drho_tor_norm2.pressure (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d2_drho_tor_norm2.pressure_fast_parallel (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d2_drho_tor_norm2.pressure_fast_perpendicular (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d2_drho_tor_norm2.temperature (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d2_drho_tor_norm2.velocity_pol (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d2_drho_tor_norm2.velocity_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_drho_tor_norm (alpha) | STRUCTURE | Derivatives with respect to the normalised toroidal flux | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_drho_tor_norm.density (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_drho_tor_norm.density_fast (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_drho_tor_norm.pressure (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_drho_tor_norm.pressure_fast_parallel (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_drho_tor_norm.pressure_fast_perpendicular (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_drho_tor_norm.temperature (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_drho_tor_norm.velocity_pol (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_drho_tor_norm.velocity_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_dt (alpha) | STRUCTURE | Derivatives with respect to time | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_dt.density (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density (thermal+non-thermal) |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_dt.density_fast (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^-3 | Density of fast (non-thermal) particles |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_dt.pressure (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Pressure |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_dt.pressure_fast_parallel (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) parallel pressure |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_dt.pressure_fast_perpendicular (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Pa | Fast (non-thermal) perpendicular pressure |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_dt.temperature (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | eV | Temperature |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_dt.velocity_pol (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Poloidal velocity |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].d_dt.velocity_tor (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Toroidal velocity |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].is_neutral (alpha) | INT_0D | Flag specifying if this state corresponds to a neutral (1) or not (0) | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].neutral_type (alpha) | STRUCTURE | Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].neutral_type.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].neutral_type.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle | |
transport_solver_numerics.derivatives_1d[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
transport_solver_numerics.derivatives_1d[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
transport_solver_numerics.derivatives_1d[:].ion[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
transport_solver_numerics.derivatives_1d[:].time (alpha) | FLT_0D | s | Time | |
transport_solver_numerics.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
transport_solver_numerics.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
transport_solver_numerics.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
transport_solver_numerics.ids_properties.occurrence | INT_0D | |||
transport_solver_numerics.primary_coordinate (alpha) | STRUCTURE | Primary coordinate system with which the transport equations are solved. For a 1D transport solver: index = 1 means rho_tor_norm; 2 = rho_tor. | ||
transport_solver_numerics.primary_coordinate.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.primary_coordinate.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.primary_coordinate.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d (alpha) | [transport_solver_numerics.profiles_1d[:].time] | STRUCT_ARRAY | Numerics related to 1D radial profiles, for various time slices | |
transport_solver_numerics.profiles_1d[:].current (alpha) | STRUCTURE | Quantities related to the current diffusion equation | ||
transport_solver_numerics.profiles_1d[:].current.boundary_condition (alpha) | STRUCTURE | Boundary condition for the current diffusion equation | ||
transport_solver_numerics.profiles_1d[:].current.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: poloidal flux; 2: ip; 3: loop voltage; 4: undefined; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].current.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].current.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].current.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].current.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].current.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].current.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 3, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].current.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].current.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].current.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].current.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].current.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].current.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].current.derivatives.d_dt_cphi (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to time, at constant toroidal flux |
transport_solver_numerics.profiles_1d[:].current.derivatives.d_dt_crho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to time, at constant normalised toroidal flux coordinate |
transport_solver_numerics.profiles_1d[:].current.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the current transport equation: index=0-psi; 1-q; 2-parallel current density | ||
transport_solver_numerics.profiles_1d[:].current.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].current.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].current.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].d_dvolume_drho_tor_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2.s^-1 | Partial derivative with respect to time of the derivative of the volume with respect to the toroidal flux coordinate |
transport_solver_numerics.profiles_1d[:].drho_tor_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m.s^-1 | Partial derivative of the toroidal flux coordinate profile with respect to time |
transport_solver_numerics.profiles_1d[:].electrons (alpha) | STRUCTURE | Quantities related to the electron transport equations | ||
transport_solver_numerics.profiles_1d[:].electrons.energy (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Numerics for the electron energy equation |
transport_solver_numerics.profiles_1d[:].electrons.energy.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates temperature) | ||
transport_solver_numerics.profiles_1d[:].electrons.energy.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].electrons.grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].electrons.energy.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].electrons.energy.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].electrons.energy.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].electrons.energy.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].electrons.energy.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].electrons.energy.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].electrons.energy.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].electrons.energy.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].electrons.energy.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].electrons.energy.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].electrons.energy.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].electrons.energy.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].electrons.energy.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (pressure for index = 0, temperature for index=1) | ||
transport_solver_numerics.profiles_1d[:].electrons.energy.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].electrons.energy.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].electrons.energy.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].electrons.particles (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Numerics for the electron density equation |
transport_solver_numerics.profiles_1d[:].electrons.particles.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates density) | ||
transport_solver_numerics.profiles_1d[:].electrons.particles.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].electrons.grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].electrons.particles.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].electrons.particles.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].electrons.particles.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].electrons.particles.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].electrons.particles.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].electrons.particles.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].electrons.particles.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].electrons.particles.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].electrons.particles.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].electrons.particles.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].electrons.particles.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].electrons.particles.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].electrons.particles.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (density for index=1) | ||
transport_solver_numerics.profiles_1d[:].electrons.particles.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].electrons.particles.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].electrons.particles.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].energy_ion_total (alpha) | [transport_solver_numerics.grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Numerics for the total ion energy equation |
transport_solver_numerics.profiles_1d[:].energy_ion_total.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates temperature) | ||
transport_solver_numerics.profiles_1d[:].energy_ion_total.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].energy_ion_total.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].energy_ion_total.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].energy_ion_total.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].energy_ion_total.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].energy_ion_total.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].energy_ion_total.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].energy_ion_total.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].energy_ion_total.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].energy_ion_total.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].energy_ion_total.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].energy_ion_total.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].energy_ion_total.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].energy_ion_total.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (pressure for index = 0, temperature for index=1) | ||
transport_solver_numerics.profiles_1d[:].energy_ion_total.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].energy_ion_total.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].energy_ion_total.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].grid (alpha) | STRUCTURE | Radial grid | ||
transport_solver_numerics.profiles_1d[:].grid.area (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
transport_solver_numerics.profiles_1d[:].grid.psi (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
transport_solver_numerics.profiles_1d[:].grid.rho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm (alpha) | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
transport_solver_numerics.profiles_1d[:].grid.volume (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
transport_solver_numerics.profiles_1d[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
transport_solver_numerics.profiles_1d[:].ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
transport_solver_numerics.profiles_1d[:].ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
transport_solver_numerics.profiles_1d[:].ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
transport_solver_numerics.profiles_1d[:].ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
transport_solver_numerics.profiles_1d[:].ion[:].energy (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Numerics for the ion energy equation |
transport_solver_numerics.profiles_1d[:].ion[:].energy.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates temperature) | ||
transport_solver_numerics.profiles_1d[:].ion[:].energy.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].ion[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].ion[:].energy.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].ion[:].energy.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].ion[:].energy.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].ion[:].energy.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].ion[:].energy.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].ion[:].energy.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].ion[:].energy.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].ion[:].energy.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].energy.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].energy.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].energy.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].energy.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].ion[:].energy.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (pressure for index = 0, temperature for index=1) | ||
transport_solver_numerics.profiles_1d[:].ion[:].energy.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].ion[:].energy.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].ion[:].energy.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].ion[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
transport_solver_numerics.profiles_1d[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
transport_solver_numerics.profiles_1d[:].ion[:].neutral_index (alpha) | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
transport_solver_numerics.profiles_1d[:].ion[:].particles (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Numerics for the ion density equation |
transport_solver_numerics.profiles_1d[:].ion[:].particles.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates density) | ||
transport_solver_numerics.profiles_1d[:].ion[:].particles.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].ion[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].ion[:].particles.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].ion[:].particles.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].ion[:].particles.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].ion[:].particles.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].ion[:].particles.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].ion[:].particles.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].ion[:].particles.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].ion[:].particles.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].particles.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].particles.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].particles.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].particles.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].ion[:].particles.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (density for index=1) | ||
transport_solver_numerics.profiles_1d[:].ion[:].particles.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].ion[:].particles.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].ion[:].particles.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].ion[:].state (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy (alpha) | [transport_solver_numerics.profiles_1d[:].ion[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Numerics for the state energy equation |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates temperature) | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].ion[:].state[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (pressure for index = 0, temperature for index=1) | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].energy.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].ionisation_potential (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Cumulative and average ionisation potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z'=0 to z-1)), where Epot is the ionisation potential of ion Xz_+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles (alpha) | [transport_solver_numerics.profiles_1d[:].ion[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Numerics for the state density equation |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates density) | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].ion[:].state[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (density for index=1) | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].particles.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
transport_solver_numerics.profiles_1d[:].ion[:].state[:].z_average (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Average Z of the charge state bundle (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle | |
transport_solver_numerics.profiles_1d[:].ion[:].state[:].z_square_average (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Average Z square of the charge state bundle (equal to z_min if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle. | |
transport_solver_numerics.profiles_1d[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed), volume averaged over plasma radius | |
transport_solver_numerics.profiles_1d[:].momentum_tor (alpha) | [transport_solver_numerics.grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Numerics for the total plasma toroidal momentum equation (summed over ion species and electrons) |
transport_solver_numerics.profiles_1d[:].momentum_tor.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates toroidal momentum) | ||
transport_solver_numerics.profiles_1d[:].momentum_tor.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].momentum_tor.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].momentum_tor.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].momentum_tor.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].momentum_tor.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].momentum_tor.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].momentum_tor.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].momentum_tor.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].momentum_tor.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].momentum_tor.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].momentum_tor.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].momentum_tor.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].momentum_tor.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].momentum_tor.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (toroidal momentum for index=1) | ||
transport_solver_numerics.profiles_1d[:].momentum_tor.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].momentum_tor.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].momentum_tor.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different neutral species | |
transport_solver_numerics.profiles_1d[:].neutral[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
transport_solver_numerics.profiles_1d[:].neutral[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
transport_solver_numerics.profiles_1d[:].neutral[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
transport_solver_numerics.profiles_1d[:].neutral[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
transport_solver_numerics.profiles_1d[:].neutral[:].energy (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Numerics for the neutral energy equation |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates temperature) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].energy.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].neutral[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].neutral[:].energy.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].energy.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral[:].energy.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].neutral[:].energy.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].neutral[:].energy.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (pressure for index = 0, temperature for index=1) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].energy.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].neutral[:].energy.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].energy.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral[:].ion_index (alpha) | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
transport_solver_numerics.profiles_1d[:].neutral[:].label (alpha) | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].multiple_states_flag (alpha) | INT_0D | Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
transport_solver_numerics.profiles_1d[:].neutral[:].particles (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Numerics for the neutral density equation |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates density) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].particles.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].neutral[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].neutral[:].particles.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].particles.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral[:].particles.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].neutral[:].particles.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].neutral[:].particles.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (density for index=1) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].particles.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].neutral[:].particles.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].particles.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy (alpha) | [transport_solver_numerics.profiles_1d[:].neutral[:].grid.rho_tor_norm] | STRUCTURE | W.m^-3 | Numerics for the state energy equation |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates temperature) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].neutral[:].state[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (pressure for index = 0, temperature for index=1) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].energy.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].label (alpha) | STR_0D | String identifying state | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].neutral_type (alpha) | STRUCTURE | Neutral type, in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].neutral_type.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].neutral_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].neutral_type.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles (alpha) | [transport_solver_numerics.profiles_1d[:].neutral[:].grid.rho_tor_norm] | STRUCTURE | m^-3.s^-1 | Numerics for the state density equation |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.boundary_condition (alpha) | STRUCTURE | Boundary condition (field y designates density) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.boundary_condition.identifier (alpha) | [transport_solver_numerics.profiles_1d[:].neutral[:].state[:].grid.rho_tor_norm] | STRUCTURE | eV | Identifier of the boundary condition type. ID = 1: value of the field y; 2: radial derivative of the field (-dy/drho_tor); 3: scale length of the field y/(-dy/drho_tor); 4: flux; 5: generic boundary condition y expressed as a1y'+a2y=a3. 6: equation not solved; |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.boundary_condition.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.boundary_condition.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.boundary_condition.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.boundary_condition.rho_tor (alpha) | FLT_0D (uncertain) | m | Position, in toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.boundary_condition.rho_tor_norm (alpha) | FLT_0D (uncertain) | - | Position, in normalised toroidal flux, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed. | |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.boundary_condition.value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For ID = 1 to 4, only the first position in the vector is used. For ID = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.derivatives (alpha) | STRUCTURE | Derivatives of the primary quantity | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.derivatives.d2_drho_tor2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.derivatives.d2_drho_tor_norm2 (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.derivatives.d_drho_tor (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.derivatives.d_drho_tor_norm (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to the normalised toroidal flux |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.derivatives.d_dt (alpha) | [transport_solver_numerics.profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.primary_quantity (alpha) | STRUCTURE | Identifier for the primary quantity of the transport equation (density for index=1) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.primary_quantity.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.primary_quantity.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].particles.primary_quantity.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
transport_solver_numerics.profiles_1d[:].neutral[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
transport_solver_numerics.profiles_1d[:].time (alpha) | FLT_0D | s | Time | |
transport_solver_numerics.restart_files (alpha) | [transport_solver_numerics.restart_files[:].time] | STRUCT_ARRAY | Set of code-specific restart files for a given time slice. These files are managed by a physical application to ensure its restart during long simulations | |
transport_solver_numerics.restart_files[:].descriptions (alpha) | [transport_solver_numerics.restart_files[:].names] | STR_1D | Descriptions of the restart files | |
transport_solver_numerics.restart_files[:].names (alpha) | [1...N] | STR_1D | Names of the restart files | |
transport_solver_numerics.restart_files[:].time (alpha) | FLT_0D | s | Time | |
transport_solver_numerics.solver (alpha) | STRUCTURE | Solver identifier | ||
transport_solver_numerics.solver.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.solver.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
transport_solver_numerics.solver.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
transport_solver_numerics.vacuum_toroidal_field (alpha) | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities) | ||
transport_solver_numerics.vacuum_toroidal_field.b0 (alpha) | [transport_solver_numerics.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
transport_solver_numerics.vacuum_toroidal_field.r0 (alpha) | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
wall (alpha) | Description of the torus wall and its interaction with the plasma | |||
wall.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
wall.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
wall.code.name (alpha) | STR_0D | Name of software generating IDS | ||
wall.code.output_flag (alpha) | [wall.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
wall.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
wall.code.repository (alpha) | STR_0D | URL of software repository | ||
wall.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
wall.description_2d (alpha) | [1...N] | STRUCT_ARRAY | Set of 2D wall descriptions, for each type of possible physics or engineering configurations necessary (gas tight vs wall with ports and holes, coarse vs fine representation, single contour limiter, disjoint gapped plasma facing components, ...). | |
wall.description_2d[:].limiter (alpha) | STRUCTURE | Description of the immobile limiting surface(s) or plasma facing components for defining the Last Closed Flux Surface. | ||
wall.description_2d[:].limiter.type (alpha) | STRUCTURE | Type of the limiter description. index = 0 for the official single contour limiter and 1 for the official disjoint PFC structure like first wall. Additional representations needed on a code-by-code basis follow same incremental pair tagging starting on flag=2 | ||
wall.description_2d[:].limiter.type.description (alpha) | STR_0D | Verbose description | ||
wall.description_2d[:].limiter.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
wall.description_2d[:].limiter.type.name (alpha) | STR_0D | Short string identifier | ||
wall.description_2d[:].limiter.unit (alpha) | [1...N] | STRUCT_ARRAY | Set of limiter units | |
wall.description_2d[:].limiter.unit[:].closed (alpha) | INT_0D | Flag identifying whether the contour is closed (1) or open (0) | ||
wall.description_2d[:].limiter.unit[:].name (alpha) | STR_0D | Name of the limiter unit | ||
wall.description_2d[:].limiter.unit[:].outline (alpha) | STRUCTURE | Irregular outline of the limiting surface. Do NOT repeat the first point for closed contours | ||
wall.description_2d[:].limiter.unit[:].outline.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
wall.description_2d[:].limiter.unit[:].outline.z (alpha) | [wall.description_2d[:].limiter.unit[:].outline.r] | FLT_1D (uncertain) | m | Height |
wall.description_2d[:].limiter.unit[:].resistivity (alpha) | FLT_0D (uncertain) | ohm.m | Resistivity of the limiter unit | |
wall.description_2d[:].type (alpha) | STRUCTURE | Type of the description. index = 0 for equilibrium codes (single closed limiter and vessel); 1 for gas-tight walls (disjoint PFCs with inner vessel as last limiter_unit; no vessel structure); 2 for free boundary codes (disjoint PFCs and vessel) | ||
wall.description_2d[:].type.description (alpha) | STR_0D | Verbose description | ||
wall.description_2d[:].type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
wall.description_2d[:].type.name (alpha) | STR_0D | Short string identifier | ||
wall.description_2d[:].vessel (alpha) | STRUCTURE | Mechanical structure of the vacuum vessel. The vessel is described as a set of nested layers with given physics properties; Two representations are admitted for each vessel unit : annular (two contours) or block elements. | ||
wall.description_2d[:].vessel.type (alpha) | STRUCTURE | Type of the vessel description. index = 0 for the official single/multiple annular vessel and 1 for the official block element representation for each vessel unit. Additional representations needed on a code-by-code basis follow same incremental pair tagging starting on flag=2 | ||
wall.description_2d[:].vessel.type.description (alpha) | STR_0D | Verbose description | ||
wall.description_2d[:].vessel.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
wall.description_2d[:].vessel.type.name (alpha) | STR_0D | Short string identifier | ||
wall.description_2d[:].vessel.unit (alpha) | [1...N] | STRUCT_ARRAY | Set of vessel units | |
wall.description_2d[:].vessel.unit[:].annular (alpha) | STRUCTURE | Annular representation of a vessel layer by two contours, inner and outer | ||
wall.description_2d[:].vessel.unit[:].annular.outline_inner (alpha) | STRUCTURE | Inner vessel outline. Do NOT repeat the first point for closed contours | ||
wall.description_2d[:].vessel.unit[:].annular.outline_inner.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
wall.description_2d[:].vessel.unit[:].annular.outline_inner.z (alpha) | [wall.description_2d[:].vessel.unit[:].annular.outline_inner.r] | FLT_1D (uncertain) | m | Height |
wall.description_2d[:].vessel.unit[:].annular.outline_outer (alpha) | STRUCTURE | Outer vessel outline. Do NOT repeat the first point for closed contours | ||
wall.description_2d[:].vessel.unit[:].annular.outline_outer.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
wall.description_2d[:].vessel.unit[:].annular.outline_outer.z (alpha) | [wall.description_2d[:].vessel.unit[:].annular.outline_outer.r] | FLT_1D (uncertain) | m | Height |
wall.description_2d[:].vessel.unit[:].annular.resistivity (alpha) | FLT_0D (uncertain) | ohm.m | Resistivity of the vessel unit | |
wall.description_2d[:].vessel.unit[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of block elements | |
wall.description_2d[:].vessel.unit[:].element[:].j_tor (alpha) | STRUCTURE | Toroidal current induced in this block element | ||
wall.description_2d[:].vessel.unit[:].element[:].j_tor.data (alpha) | [wall.description_2d[:].vessel.unit[:].element[:].j_tor.time] | FLT_1D (uncertain) | A | Toroidal current induced in this block element |
wall.description_2d[:].vessel.unit[:].element[:].j_tor.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
wall.description_2d[:].vessel.unit[:].element[:].name (alpha) | STR_0D | Name of the block element | ||
wall.description_2d[:].vessel.unit[:].element[:].outline (alpha) | STRUCTURE | Outline of the block element. Do NOT repeat the first point for closed contours | ||
wall.description_2d[:].vessel.unit[:].element[:].outline.r (alpha) | [1...N] | FLT_1D (uncertain) | m | Major radius |
wall.description_2d[:].vessel.unit[:].element[:].outline.z (alpha) | [wall.description_2d[:].vessel.unit[:].element[:].outline.r] | FLT_1D (uncertain) | m | Height |
wall.description_2d[:].vessel.unit[:].element[:].resistance (alpha) | FLT_0D (uncertain) | Ohm | Resistance of the block element | |
wall.description_2d[:].vessel.unit[:].element[:].resistivity (alpha) | FLT_0D (uncertain) | ohm.m | Resistivity of the block element | |
wall.description_2d[:].vessel.unit[:].name (alpha) | STR_0D | Name of the vessel unit | ||
wall.global_quantities (alpha) | STRUCTURE | Simple 0D description of plasma-wall interaction | ||
wall.global_quantities.electrons (alpha) | STRUCTURE | Quantities related to electrons | ||
wall.global_quantities.electrons.gas_puff (alpha) | [wall.time] | FLT_1D (uncertain) | s^-1 | Gas puff rate (in equivalent electrons) |
wall.global_quantities.electrons.particle_flux_from_plasma (alpha) | [wall.time] | FLT_1D (uncertain) | s^-1 | Particle flux from the plasma (in equivalent electrons) |
wall.global_quantities.electrons.particle_flux_from_wall (alpha) | [1...3, | FLT_2D (uncertain) | s^-1 | Particle flux from the wall corresponding to the conversion into various neutral types (first dimension: 1: cold; 2: thermal; 3: fast), in equivalent electrons |
wall.global_quantities.electrons.pumping_speed (alpha) | [wall.time] | FLT_1D (uncertain) | s^-1 | Pumped particle flux (in equivalent electrons) |
wall.global_quantities.neutral (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the various neutral species | |
wall.global_quantities.neutral[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
wall.global_quantities.neutral[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
wall.global_quantities.neutral[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
wall.global_quantities.neutral[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
wall.global_quantities.neutral[:].gas_puff (alpha) | [wall.time] | FLT_1D (uncertain) | s^-1 | Gas puff rate for that species |
wall.global_quantities.neutral[:].label (alpha) | STR_0D | String identifying the species (e.g. H, D, CD4, ...) | ||
wall.global_quantities.neutral[:].particle_flux_from_plasma (alpha) | [wall.time] | FLT_1D (uncertain) | s^-1 | Particle flux from the plasma for that species |
wall.global_quantities.neutral[:].particle_flux_from_wall (alpha) | [1...3, | FLT_2D (uncertain) | s^-1 | Particle flux from the wall corresponding to the conversion into various neutral types (first dimension: 1: cold; 2: thermal; 3: fast) |
wall.global_quantities.neutral[:].pumping_speed (alpha) | [wall.time] | FLT_1D (uncertain) | s^-1 | Pumped particle flux for that species |
wall.global_quantities.neutral[:].recycling_energy_coefficient (alpha) | [1...3, | FLT_2D (uncertain) | - | Energy recycling coefficient corresponding to the conversion into various neutral types (first dimension: 1: cold; 2: thermal; 3: fast) |
wall.global_quantities.neutral[:].recycling_particles_coefficient (alpha) | [1...3, | FLT_2D (uncertain) | - | Particle recycling coefficient corresponding to the conversion into various neutral types (first dimension: 1: cold; 2: thermal; 3: fast) |
wall.global_quantities.neutral[:].sputtering_chemical_coefficient (alpha) | [1...3, | FLT_2D (uncertain) | - | Effective coefficient of chemical sputtering for various neutral types (first dimension: 1: cold; 2: thermal; 3: fast) |
wall.global_quantities.neutral[:].sputtering_physical_coefficient (alpha) | [1...3, | FLT_2D (uncertain) | - | Effective coefficient of physical sputtering for various neutral types (first dimension: 1: cold; 2: thermal; 3: fast) |
wall.global_quantities.neutral[:].wall_inventory (alpha) | [wall.time] | FLT_1D (uncertain) | - | Wall inventory, i.e. cumulated exchange of neutral species between plasma and wall from t = 0, positive if a species has gone to the wall, for that species |
wall.global_quantities.power_from_plasma (alpha) | [wall.time] | FLT_1D (uncertain) | W | Power flowing from the plasma to the wall |
wall.global_quantities.power_to_cooling (alpha) | [wall.time] | FLT_1D (uncertain) | W | Power to cooling systems |
wall.global_quantities.temperature (alpha) | [wall.time] | FLT_1D (uncertain) | K | Wall temperature |
wall.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
wall.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
wall.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
wall.ids_properties.occurrence | INT_0D | |||
wall.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] |
| Path | Dimensions | Type | Units | Description |
|---|---|---|---|---|
waves (alpha) | RF wave propagation and deposition | |||
waves.code (alpha) | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
waves.code.commit (alpha) | STR_0D | Unique commit reference of software | ||
waves.code.name (alpha) | STR_0D | Name of software generating IDS | ||
waves.code.output_flag (alpha) | [waves.time] | INT_1D | Output flag : 0 means the run is successful, other values mean some difficulty has been encountered, the exact meaning is then code specific. Negative values mean the result shall not be used. | |
waves.code.parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
waves.code.repository (alpha) | STR_0D | URL of software repository | ||
waves.code.version (alpha) | STR_0D | Unique version (tag) of software | ||
waves.coherent_wave (alpha) | [1...N] | STRUCT_ARRAY | Wave description for each frequency | |
waves.coherent_wave[:].beam_tracing (alpha) | [waves.coherent_wave[:].beam_tracing[:].time] | STRUCT_ARRAY | Beam tracing calculations, for various time slices | |
waves.coherent_wave[:].beam_tracing[:].beam (alpha) | [1...N] | STRUCT_ARRAY | Set of rays/beams describing the wave propagation | |
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field (alpha) | STRUCTURE | Electric field polarization of the ray/beam along its path | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field.minus (alpha) | STRUCTURE | V.m^-1 | Right hand polarised electric field component | |
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field.minus.imaginary (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | V.m^-1 | Imaginary part |
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field.minus.real (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | V.m^-1 | Real part |
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field.parallel (alpha) | STRUCTURE | V.m^-1 | Parallel to magnetic field polarised electric field component | |
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field.parallel.imaginary (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | V.m^-1 | Imaginary part |
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field.parallel.real (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | V.m^-1 | Real part |
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field.plus (alpha) | STRUCTURE | V.m^-1 | Left hand polarised electric field component | |
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field.plus.imaginary (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | V.m^-1 | Imaginary part |
waves.coherent_wave[:].beam_tracing[:].beam[:].e_field.plus.real (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | V.m^-1 | Real part |
waves.coherent_wave[:].beam_tracing[:].beam[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].electrons.power (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | W | Power absorbed along the beam by the species |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].power (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | W | Power absorbed along the beam by the species |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].state[:].power (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | W | Power absorbed along the beam by the species |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
waves.coherent_wave[:].beam_tracing[:].beam[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
waves.coherent_wave[:].beam_tracing[:].beam[:].length (alpha) | [1...N] | FLT_1D (uncertain) | m | Ray/beam curvilinear length |
waves.coherent_wave[:].beam_tracing[:].beam[:].position (alpha) | STRUCTURE | Position of the ray/beam along its path | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].position.phi (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | rad | Toroidal angle |
waves.coherent_wave[:].beam_tracing[:].beam[:].position.psi (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | Wb | Poloidal flux |
waves.coherent_wave[:].beam_tracing[:].beam[:].position.r (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | m | Major radius |
waves.coherent_wave[:].beam_tracing[:].beam[:].position.theta (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | rad | Poloidal angle |
waves.coherent_wave[:].beam_tracing[:].beam[:].position.z (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | m | Height |
waves.coherent_wave[:].beam_tracing[:].beam[:].power_flow_norm (alpha) | STRUCTURE | Normalised power flow | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].power_flow_norm.parallel (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | - | Normalized power flow in the direction parallel to the magnetic field |
waves.coherent_wave[:].beam_tracing[:].beam[:].power_flow_norm.perpendicular (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | - | Normalized power flow in the direction perpendicular to the magnetic field |
waves.coherent_wave[:].beam_tracing[:].beam[:].power_initial (alpha) | FLT_0D (uncertain) | W | Initial power in the ray/beam | |
waves.coherent_wave[:].beam_tracing[:].beam[:].wave_vector (alpha) | STRUCTURE | Wave vector of the ray/beam along its path | ||
waves.coherent_wave[:].beam_tracing[:].beam[:].wave_vector.k_r (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | m^-1 | Wave vector component in the major radius direction |
waves.coherent_wave[:].beam_tracing[:].beam[:].wave_vector.k_tor (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | m^-1 | Wave vector component in the toroidal direction |
waves.coherent_wave[:].beam_tracing[:].beam[:].wave_vector.k_z (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | m^-1 | Wave vector component in the vertical direction |
waves.coherent_wave[:].beam_tracing[:].beam[:].wave_vector.n_parallel (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | - | Parallel refractive index |
waves.coherent_wave[:].beam_tracing[:].beam[:].wave_vector.n_perpendicular (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | FLT_1D (uncertain) | - | Perpendicular refractive index |
waves.coherent_wave[:].beam_tracing[:].beam[:].wave_vector.n_tor (alpha) | [waves.coherent_wave[:].beam_tracing[:].beam[:].length] | INT_1D | Toroidal wave number, contains a single value if varying_ntor = 1 to avoid useless repetition constant values | |
waves.coherent_wave[:].beam_tracing[:].beam[:].wave_vector.varying_n_tor (alpha) | INT_0D | Flag telling whether n_tor is constant along the ray path (0) or varying (1) | ||
waves.coherent_wave[:].beam_tracing[:].time (alpha) | FLT_0D | s | Time | |
waves.coherent_wave[:].full_wave (alpha) | [waves.coherent_wave[:].full_wave[:].time] | STRUCT_ARRAY | Solution by a full wave code, given on a generic grid description, for various time slices | |
waves.coherent_wave[:].full_wave[:].b_field (alpha) | STRUCTURE | Components of the wave magnetic field | ||
waves.coherent_wave[:].full_wave[:].b_field.bi_normal (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Magnitude of perpendicular (to the static magnetic field) wave magnetic field tangent to a flux surface, given on various grid subsets |
waves.coherent_wave[:].full_wave[:].b_field.bi_normal[:].coefficients (alpha) | [waves.coherent_wave[:].full_wave[:].b_field.bi_normal[:].values, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
waves.coherent_wave[:].full_wave[:].b_field.bi_normal[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
waves.coherent_wave[:].full_wave[:].b_field.bi_normal[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
waves.coherent_wave[:].full_wave[:].b_field.bi_normal[:].values (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | One scalar value is provided per element in the grid subset. |
waves.coherent_wave[:].full_wave[:].b_field.normal (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Magnitude of wave magnetic field normal to a flux surface, given on various grid subsets |
waves.coherent_wave[:].full_wave[:].b_field.normal[:].coefficients (alpha) | [waves.coherent_wave[:].full_wave[:].b_field.normal[:].values, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
waves.coherent_wave[:].full_wave[:].b_field.normal[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
waves.coherent_wave[:].full_wave[:].b_field.normal[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
waves.coherent_wave[:].full_wave[:].b_field.normal[:].values (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | One scalar value is provided per element in the grid subset. |
waves.coherent_wave[:].full_wave[:].b_field.parallel (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Parallel (to the static magnetic field) component of the wave magnetic field, given on various grid subsets |
waves.coherent_wave[:].full_wave[:].b_field.parallel[:].coefficients (alpha) | [waves.coherent_wave[:].full_wave[:].b_field.parallel[:].values, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
waves.coherent_wave[:].full_wave[:].b_field.parallel[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
waves.coherent_wave[:].full_wave[:].b_field.parallel[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
waves.coherent_wave[:].full_wave[:].b_field.parallel[:].values (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | One scalar value is provided per element in the grid subset. |
waves.coherent_wave[:].full_wave[:].e_field (alpha) | STRUCTURE | Components of the wave electric field | ||
waves.coherent_wave[:].full_wave[:].e_field.bi_normal (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Magnitude of perpendicular (to the static magnetic field) wave electric field tangent to a flux surface, given on various grid subsets |
waves.coherent_wave[:].full_wave[:].e_field.bi_normal[:].coefficients (alpha) | [waves.coherent_wave[:].full_wave[:].e_field.bi_normal[:].values, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
waves.coherent_wave[:].full_wave[:].e_field.bi_normal[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
waves.coherent_wave[:].full_wave[:].e_field.bi_normal[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
waves.coherent_wave[:].full_wave[:].e_field.bi_normal[:].values (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | One scalar value is provided per element in the grid subset. |
waves.coherent_wave[:].full_wave[:].e_field.minus (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Right hand circularly polarised component of the perpendicular (to the static magnetic field) electric field, given on various grid subsets |
waves.coherent_wave[:].full_wave[:].e_field.minus[:].coefficients (alpha) | [waves.coherent_wave[:].full_wave[:].e_field.minus[:].values, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
waves.coherent_wave[:].full_wave[:].e_field.minus[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
waves.coherent_wave[:].full_wave[:].e_field.minus[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
waves.coherent_wave[:].full_wave[:].e_field.minus[:].values (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | One scalar value is provided per element in the grid subset. |
waves.coherent_wave[:].full_wave[:].e_field.normal (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Magnitude of wave electric field normal to a flux surface, given on various grid subsets |
waves.coherent_wave[:].full_wave[:].e_field.normal[:].coefficients (alpha) | [waves.coherent_wave[:].full_wave[:].e_field.normal[:].values, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
waves.coherent_wave[:].full_wave[:].e_field.normal[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
waves.coherent_wave[:].full_wave[:].e_field.normal[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
waves.coherent_wave[:].full_wave[:].e_field.normal[:].values (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | One scalar value is provided per element in the grid subset. |
waves.coherent_wave[:].full_wave[:].e_field.parallel (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Parallel (to the static magnetic field) component of electric field, given on various grid subsets |
waves.coherent_wave[:].full_wave[:].e_field.parallel[:].coefficients (alpha) | [waves.coherent_wave[:].full_wave[:].e_field.parallel[:].values, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
waves.coherent_wave[:].full_wave[:].e_field.parallel[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
waves.coherent_wave[:].full_wave[:].e_field.parallel[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
waves.coherent_wave[:].full_wave[:].e_field.parallel[:].values (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | One scalar value is provided per element in the grid subset. |
waves.coherent_wave[:].full_wave[:].e_field.plus (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Left hand circularly polarised component of the perpendicular (to the static magnetic field) electric field, given on various grid subsets |
waves.coherent_wave[:].full_wave[:].e_field.plus[:].coefficients (alpha) | [waves.coherent_wave[:].full_wave[:].e_field.plus[:].values, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
waves.coherent_wave[:].full_wave[:].e_field.plus[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
waves.coherent_wave[:].full_wave[:].e_field.plus[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
waves.coherent_wave[:].full_wave[:].e_field.plus[:].values (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | One scalar value is provided per element in the grid subset. |
waves.coherent_wave[:].full_wave[:].grid (alpha) | STRUCTURE | Grid description | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset (alpha) | [1...N] | STRUCT_ARRAY | Grid subsets | |
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].base (alpha) | [1...N] | STRUCT_ARRAY | Set of bases for the grid subset. For each base, the structure describes the projection of the base vectors on the canonical frame of the grid. | |
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].base[:].jacobian (alpha) | [waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].base[:].tensor_contravariant (alpha) | [waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].base[:].tensor_covariant (alpha) | [waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].dimension (alpha) | INT_0D | Space dimension of the grid subset elements. This must be equal to the sum of the dimensions of the individual objects forming the element. | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element (alpha) | [1...N] | STRUCT_ARRAY | Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces | |
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element[:].object[:].dimension (alpha) | INT_0D | Dimension of the object | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element[:].object[:].index (alpha) | INT_0D | Object index | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element[:].object[:].space (alpha) | INT_0D | Index of the space from which that object is taken | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].identifier (alpha) | STRUCTURE | Grid subset identifier | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].identifier.description (alpha) | STR_0D | Verbose description | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].identifier.name (alpha) | STR_0D | Short string identifier | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].metric (alpha) | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].metric.jacobian (alpha) | [waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].metric.tensor_contravariant (alpha) | [waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].metric.tensor_covariant (alpha) | [waves.coherent_wave[:].full_wave[:].grid.grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
waves.coherent_wave[:].full_wave[:].grid.identifier (alpha) | STRUCTURE | Grid identifier | ||
waves.coherent_wave[:].full_wave[:].grid.identifier.description (alpha) | STR_0D | Verbose description | ||
waves.coherent_wave[:].full_wave[:].grid.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
waves.coherent_wave[:].full_wave[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
waves.coherent_wave[:].full_wave[:].grid.space (alpha) | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
waves.coherent_wave[:].full_wave[:].grid.space[:].coordinates_type (alpha) | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therfore defines the dimension of the space. The meaning of these predefined integer constants can be found in the documentation of the grid service library | |
waves.coherent_wave[:].full_wave[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier) | ||
waves.coherent_wave[:].full_wave[:].grid.space[:].geometry_type.description (alpha) | STR_0D | Verbose description | ||
waves.coherent_wave[:].full_wave[:].grid.space[:].geometry_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
waves.coherent_wave[:].full_wave[:].grid.space[:].geometry_type.name (alpha) | STR_0D | Short string identifier | ||
waves.coherent_wave[:].full_wave[:].grid.space[:].objects_per_dimension (alpha) | [1...N] | STRUCT_ARRAY | Definition of the space objects for every dimension (from one to the dimension of the highest-dimensional objects). The index correspond to 1=nodes, 2=edges, 3=faces, 4=cells/volumes, .... For every index, a collection of objects of that dimension is described. | |
waves.coherent_wave[:].full_wave[:].grid.space[:].objects_per_dimension[:].object (alpha) | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
waves.coherent_wave[:].full_wave[:].grid.space[:].objects_per_dimension[:].object[:].boundary (alpha) | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
waves.coherent_wave[:].full_wave[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].index (alpha) | INT_0D | Index of this (n-1)-dimensional boundary object | ||
waves.coherent_wave[:].full_wave[:].grid.space[:].objects_per_dimension[:].object[:].boundary[:].neighbours (alpha) | [1...N] | INT_1D | List of indices of the n-dimensional objects adjacent to the given n-dimensional object. An object can possibly have multiple neighbours on a boundary | |
waves.coherent_wave[:].full_wave[:].grid.space[:].objects_per_dimension[:].object[:].geometry (alpha) | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. |
waves.coherent_wave[:].full_wave[:].grid.space[:].objects_per_dimension[:].object[:].measure (alpha) | FLT_0D (uncertain) | m^dimension | Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,...) | |
waves.coherent_wave[:].full_wave[:].grid.space[:].objects_per_dimension[:].object[:].nodes (alpha) | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
waves.coherent_wave[:].full_wave[:].k_perpendicular (alpha) | [1...N] | STRUCT_ARRAY | V.m^-1 | Perpendicular wave vector, given on various grid subsets |
waves.coherent_wave[:].full_wave[:].k_perpendicular[:].coefficients (alpha) | [waves.coherent_wave[:].full_wave[:].k_perpendicular[:].values, | FLT_2D (uncertain) | V.m^-1 | Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension). |
waves.coherent_wave[:].full_wave[:].k_perpendicular[:].grid_index (alpha) | INT_0D | Index of the grid used to represent this quantity | ||
waves.coherent_wave[:].full_wave[:].k_perpendicular[:].grid_subset_index (alpha) | INT_0D | Index of the grid subset the data is provided on | ||
waves.coherent_wave[:].full_wave[:].k_perpendicular[:].values (alpha) | [1...N] | FLT_1D (uncertain) | V.m^-1 | One scalar value is provided per element in the grid subset. |
waves.coherent_wave[:].full_wave[:].time (alpha) | FLT_0D | s | Time | |
waves.coherent_wave[:].global_quantities (alpha) | [waves.coherent_wave[:].global_quantities[:].time] | STRUCT_ARRAY | Global quantities for various time slices | |
waves.coherent_wave[:].global_quantities[:].current_tor (alpha) | FLT_0D (uncertain) | A | Wave driven toroidal current from a stand alone calculation (not consistent with other sources) | |
waves.coherent_wave[:].global_quantities[:].current_tor_n_tor (alpha) | [waves.coherent_wave[:].global_quantities[:].n_tor] | FLT_1D (uncertain) | A | Wave driven toroidal current from a stand alone calculation (not consistent with other sources) per toroidal mode number |
waves.coherent_wave[:].global_quantities[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
waves.coherent_wave[:].global_quantities[:].electrons.distribution_assumption (alpha) | INT_0D | Assumption on the distribution function used by the wave solver to calculate the power deposition on this species: 0 = Maxwellian (linear absorption); 1 = quasi-linear (F given by a distributions IDS). | ||
waves.coherent_wave[:].global_quantities[:].electrons.power_fast (alpha) | FLT_0D (uncertain) | W | Wave power absorbed by the fast particle population | |
waves.coherent_wave[:].global_quantities[:].electrons.power_fast_n_tor (alpha) | [waves.coherent_wave[:].global_quantities[:].n_tor] | FLT_1D (uncertain) | W | Wave power absorbed by the fast particle population per toroidal mode number |
waves.coherent_wave[:].global_quantities[:].electrons.power_thermal (alpha) | FLT_0D (uncertain) | W | Wave power absorbed by the thermal particle population | |
waves.coherent_wave[:].global_quantities[:].electrons.power_thermal_n_tor (alpha) | [waves.coherent_wave[:].global_quantities[:].n_tor] | FLT_1D (uncertain) | W | Wave power absorbed by the thermal particle population per toroidal mode number |
waves.coherent_wave[:].global_quantities[:].frequency (alpha) | FLT_0D (uncertain) | Hz | Wave frequency | |
waves.coherent_wave[:].global_quantities[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
waves.coherent_wave[:].global_quantities[:].ion[:].distribution_assumption (alpha) | INT_0D | Assumption on the distribution function used by the wave solver to calculate the power deposition on this species: 0 = Maxwellian (linear absorption); 1 = quasi-linear (F given by a distributions IDS). | ||
waves.coherent_wave[:].global_quantities[:].ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
waves.coherent_wave[:].global_quantities[:].ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
waves.coherent_wave[:].global_quantities[:].ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
waves.coherent_wave[:].global_quantities[:].ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
waves.coherent_wave[:].global_quantities[:].ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
waves.coherent_wave[:].global_quantities[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
waves.coherent_wave[:].global_quantities[:].ion[:].power_fast (alpha) | FLT_0D (uncertain) | W | Wave power absorbed by the fast particle population | |
waves.coherent_wave[:].global_quantities[:].ion[:].power_fast_n_tor (alpha) | [waves.coherent_wave[:].global_quantities[:].n_tor] | FLT_1D (uncertain) | W | Wave power absorbed by the fast particle population per toroidal mode number |
waves.coherent_wave[:].global_quantities[:].ion[:].power_thermal (alpha) | FLT_0D (uncertain) | W | Wave power absorbed by the thermal particle population | |
waves.coherent_wave[:].global_quantities[:].ion[:].power_thermal_n_tor (alpha) | [waves.coherent_wave[:].global_quantities[:].n_tor] | FLT_1D (uncertain) | W | Wave power absorbed by the thermal particle population per toroidal mode number |
waves.coherent_wave[:].global_quantities[:].ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].power_fast (alpha) | FLT_0D (uncertain) | W | Wave power absorbed by the fast particle population | |
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].power_fast_n_tor (alpha) | [waves.coherent_wave[:].global_quantities[:].n_tor] | FLT_1D (uncertain) | W | Wave power absorbed by the fast particle population per toroidal mode number |
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].power_thermal (alpha) | FLT_0D (uncertain) | W | Wave power absorbed by the thermal particle population | |
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].power_thermal_n_tor (alpha) | [waves.coherent_wave[:].global_quantities[:].n_tor] | FLT_1D (uncertain) | W | Wave power absorbed by the thermal particle population per toroidal mode number |
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
waves.coherent_wave[:].global_quantities[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
waves.coherent_wave[:].global_quantities[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
waves.coherent_wave[:].global_quantities[:].n_tor (alpha) | [1...N] | INT_1D | Toroidal mode numbers | |
waves.coherent_wave[:].global_quantities[:].power (alpha) | FLT_0D (uncertain) | W | Total absorbed wave power | |
waves.coherent_wave[:].global_quantities[:].power_n_tor (alpha) | [waves.coherent_wave[:].global_quantities[:].n_tor] | FLT_1D (uncertain) | W | Absorbed wave power per toroidal mode number |
waves.coherent_wave[:].global_quantities[:].time (alpha) | FLT_0D | s | Time | |
waves.coherent_wave[:].identifier (alpha) | STRUCTURE | Identifier of the coherent wave, in terms of the type and name of the antenna driving the wave and an index separating waves driven by the same antenna. | ||
waves.coherent_wave[:].identifier.antenna_name (alpha) | STR_0D | Name of the antenna that launches this wave. Corresponds to the name specified in antennas/ec(i)/name, or antennas/ic(i)/name or antennas/lh(i)/name (depends of antenna/wave type) in the ANTENNAS IDS. | ||
waves.coherent_wave[:].identifier.index_in_antenna (alpha) | INT_0D | Index of the wave (starts at 1), separating different waves generated from a single antenna. | ||
waves.coherent_wave[:].identifier.type (alpha) | STRUCTURE | Wave/antenna type. index=1 for name=EC; index=2 for name=IC; index=3 for name=LH | ||
waves.coherent_wave[:].identifier.type.description (alpha) | STR_0D | Verbose description | ||
waves.coherent_wave[:].identifier.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
waves.coherent_wave[:].identifier.type.name (alpha) | STR_0D | Short string identifier | ||
waves.coherent_wave[:].profiles_1d (alpha) | [waves.coherent_wave[:].profiles_1d[:].time] | STRUCT_ARRAY | Source radial profiles (flux surface averaged quantities) for various time slices | |
waves.coherent_wave[:].profiles_1d[:].current_parallel_density (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A.m^-2 | Flux surface averaged wave driven parallel current density = average(j.B) / B0, where B0 = vacuum_toroidal_field/b0. |
waves.coherent_wave[:].profiles_1d[:].current_parallel_density_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | A.m^-2 | Flux surface averaged wave driven parallel current density, per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].current_tor_inside (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | A | Wave driven toroidal current from a stand alone calculation (not consistent with other sources), inside a flux surface |
waves.coherent_wave[:].profiles_1d[:].current_tor_inside_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | A | Wave driven toroidal current from a stand alone calculation (not consistent with other sources), inside a flux surface, per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].n_tor] | STRUCT_ARRAY | Components of the electric field per toroidal mode number, averaged over the flux surface, where the averaged is weighted with the power deposition density, such that e_field = ave(e_field.power_density) / ave(power_density) | |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor[:].minus (alpha) | STRUCTURE | V.m^-1 | Right hand polarised electric field component for every flux surface | |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor[:].minus.amplitude (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Amplitude |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor[:].minus.phase (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Phase |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor[:].parallel (alpha) | STRUCTURE | V.m^-1 | Parallel electric field component for every flux surface | |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor[:].parallel.amplitude (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Amplitude |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor[:].parallel.phase (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Phase |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor[:].plus (alpha) | STRUCTURE | V.m^-1 | Left hand polarised electric field component for every flux surface | |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor[:].plus.amplitude (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Amplitude |
waves.coherent_wave[:].profiles_1d[:].e_field_n_tor[:].plus.phase (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | V.m^-1 | Phase |
waves.coherent_wave[:].profiles_1d[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
waves.coherent_wave[:].profiles_1d[:].electrons.power_density_fast (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the fast species |
waves.coherent_wave[:].profiles_1d[:].electrons.power_density_fast_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the fast species, per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].electrons.power_density_thermal (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the thermal species |
waves.coherent_wave[:].profiles_1d[:].electrons.power_density_thermal_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the thermal species, per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].electrons.power_inside_fast (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density) |
waves.coherent_wave[:].profiles_1d[:].electrons.power_inside_fast_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density), per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].electrons.power_inside_thermal (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density) |
waves.coherent_wave[:].profiles_1d[:].electrons.power_inside_thermal_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density), per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].grid (alpha) | STRUCTURE | Radial grid | ||
waves.coherent_wave[:].profiles_1d[:].grid.area (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
waves.coherent_wave[:].profiles_1d[:].grid.psi (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
waves.coherent_wave[:].profiles_1d[:].grid.rho_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m | Toroidal flux coordinate. rho_tor = sqrt(b_flux_tor/(pi*b0)) ~ sqrt(pi*r^2*b0/(pi*b0)) ~ r [m]. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm (alpha) | [1...N] | FLT_1D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation, see time_slice/boundary/b_flux_pol_norm in the equilibrium IDS) |
waves.coherent_wave[:].profiles_1d[:].grid.volume (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
waves.coherent_wave[:].profiles_1d[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
waves.coherent_wave[:].profiles_1d[:].ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
waves.coherent_wave[:].profiles_1d[:].ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
waves.coherent_wave[:].profiles_1d[:].ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
waves.coherent_wave[:].profiles_1d[:].ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
waves.coherent_wave[:].profiles_1d[:].ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
waves.coherent_wave[:].profiles_1d[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
waves.coherent_wave[:].profiles_1d[:].ion[:].power_density_fast (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the fast species |
waves.coherent_wave[:].profiles_1d[:].ion[:].power_density_fast_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the fast species, per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].ion[:].power_density_thermal (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the thermal species |
waves.coherent_wave[:].profiles_1d[:].ion[:].power_density_thermal_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the thermal species, per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].ion[:].power_inside_fast (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density) |
waves.coherent_wave[:].profiles_1d[:].ion[:].power_inside_fast_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density), per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].ion[:].power_inside_thermal (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density) |
waves.coherent_wave[:].profiles_1d[:].ion[:].power_inside_thermal_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density), per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].power_density_fast (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the fast species |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].power_density_fast_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the fast species, per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].power_density_thermal (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the thermal species |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].power_density_thermal_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density on the thermal species, per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].power_inside_fast (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density) |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].power_inside_fast_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density), per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].power_inside_thermal (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density) |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].power_inside_thermal_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W | Absorbed wave power on thermal species inside a flux surface (cumulative volume integral of the absorbed power density), per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
waves.coherent_wave[:].profiles_1d[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
waves.coherent_wave[:].profiles_1d[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
waves.coherent_wave[:].profiles_1d[:].k_perpendicular (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | V.m^-1 | Perpendicular wave vector, averaged over the flux surface, where the averaged is weighted with the power deposition density, such that k_perpendicular = ave(k_perpendicular.power_density) / ave(power_density), for every flux surface and every toroidal number |
waves.coherent_wave[:].profiles_1d[:].n_tor (alpha) | [1...N] | INT_1D | Toroidal mode numbers | |
waves.coherent_wave[:].profiles_1d[:].power_density (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W.m^-3 | Flux surface averaged total absorbed wave power density (electrons + ion + fast populations) |
waves.coherent_wave[:].profiles_1d[:].power_density_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W.m^-3 | Flux surface averaged absorbed wave power density per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].power_inside (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | W | Total absorbed wave power (electrons + ion + fast populations) inside a flux surface (cumulative volume integral of the absorbed power density) |
waves.coherent_wave[:].profiles_1d[:].power_inside_n_tor (alpha) | [waves.coherent_wave[:].profiles_1d[:].grid.rho_tor_norm, | FLT_2D (uncertain) | W | Total absorbed wave power (electrons + ion + fast populations) inside a flux surface (cumulative volume integral of the absorbed power density), per toroidal mode number |
waves.coherent_wave[:].profiles_1d[:].time (alpha) | FLT_0D | s | Time | |
waves.coherent_wave[:].profiles_2d (alpha) | [waves.coherent_wave[:].profiles_2d[:].time] | STRUCT_ARRAY | 2D profiles in poloidal cross-section, for various time slices | |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor (alpha) | [waves.coherent_wave[:].profiles_2d[:].n_tor] | STRUCT_ARRAY | Components of the electric field per toroidal mode number | |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor[:].minus (alpha) | STRUCTURE | V.m^-1 | Right hand polarised electric field component | |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor[:].minus.amplitude (alpha) | [1...N, | FLT_2D (uncertain) | V.m^-1 | Amplitude |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor[:].minus.phase (alpha) | [1...N, | FLT_2D (uncertain) | V.m^-1 | Phase |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor[:].parallel (alpha) | STRUCTURE | V.m^-1 | Parallel electric field component | |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor[:].parallel.amplitude (alpha) | [1...N, | FLT_2D (uncertain) | V.m^-1 | Amplitude |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor[:].parallel.phase (alpha) | [1...N, | FLT_2D (uncertain) | V.m^-1 | Phase |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor[:].plus (alpha) | STRUCTURE | V.m^-1 | Left hand polarised electric field component | |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor[:].plus.amplitude (alpha) | [1...N, | FLT_2D (uncertain) | V.m^-1 | Amplitude |
waves.coherent_wave[:].profiles_2d[:].e_field_n_tor[:].plus.phase (alpha) | [1...N, | FLT_2D (uncertain) | V.m^-1 | Phase |
waves.coherent_wave[:].profiles_2d[:].electrons (alpha) | STRUCTURE | Quantities related to the electrons | ||
waves.coherent_wave[:].profiles_2d[:].electrons.power_density_fast (alpha) | [1...N, | FLT_2D (uncertain) | W.m^-3 | Absorbed wave power density on the fast species |
waves.coherent_wave[:].profiles_2d[:].electrons.power_density_fast_n_tor (alpha) | [1...N, | FLT_3D (uncertain) | W.m^-3 | Absorbed wave power density on the fast species, per toroidal mode number |
waves.coherent_wave[:].profiles_2d[:].electrons.power_density_thermal (alpha) | [1...N, | FLT_2D (uncertain) | W.m^-3 | Absorbed wave power density on the thermal species |
waves.coherent_wave[:].profiles_2d[:].electrons.power_density_thermal_n_tor (alpha) | [1...N, | FLT_3D (uncertain) | W.m^-3 | Absorbed wave power density on the thermal species, per toroidal mode number |
waves.coherent_wave[:].profiles_2d[:].grid (alpha) | STRUCTURE | 2D grid in a poloidal cross-section | ||
waves.coherent_wave[:].profiles_2d[:].grid.area (alpha) | [1...N, | FLT_2D (uncertain) | m^2 | Cross-sectional area of the flux surface |
waves.coherent_wave[:].profiles_2d[:].grid.psi (alpha) | [1...N, | FLT_2D (uncertain) | Wb | Poloidal magnetic flux |
waves.coherent_wave[:].profiles_2d[:].grid.r (alpha) | [1...N, | FLT_2D (uncertain) | m | Major radius |
waves.coherent_wave[:].profiles_2d[:].grid.rho_tor (alpha) | [1...N, | FLT_2D (uncertain) | m | Toroidal flux coordinate. The toroidal field used in its definition is indicated under vacuum_toroidal_field/b0 |
waves.coherent_wave[:].profiles_2d[:].grid.rho_tor_norm (alpha) | [1...N, | FLT_2D (uncertain) | - | Normalised toroidal flux coordinate. The normalizing value for rho_tor_norm, is the toroidal flux coordinate at the equilibrium boundary (LCFS or 99.x % of the LCFS in case of a fixed boundary equilibium calculation) |
waves.coherent_wave[:].profiles_2d[:].grid.theta_geometric (alpha) | [1...N, | FLT_2D (uncertain) | rad | Geometrical poloidal angle |
waves.coherent_wave[:].profiles_2d[:].grid.theta_straight (alpha) | [1...N, | FLT_2D (uncertain) | rad | Straight field line poloidal angle |
waves.coherent_wave[:].profiles_2d[:].grid.type (alpha) | [waves.coherent_wave[:].profiles_2d[:].grid.rho_tor_norm] | STRUCTURE | m^3 | Grid type: index=0: Rectangular grid in the (R,Z) coordinates; index=1: Rectangular grid in the (radial, theta_geometric) coordinates; index=2: Rectangular grid in the (radial, theta_straight) coordinates. index=3: unstructured grid. |
waves.coherent_wave[:].profiles_2d[:].grid.type.description (alpha) | STR_0D | Verbose description | ||
waves.coherent_wave[:].profiles_2d[:].grid.type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
waves.coherent_wave[:].profiles_2d[:].grid.type.name (alpha) | STR_0D | Short string identifier | ||
waves.coherent_wave[:].profiles_2d[:].grid.volume (alpha) | [1...N, | FLT_2D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
waves.coherent_wave[:].profiles_2d[:].grid.z (alpha) | [1...N, | FLT_2D (uncertain) | m | Height |
waves.coherent_wave[:].profiles_2d[:].ion (alpha) | [1...N] | STRUCT_ARRAY | Quantities related to the different ion species | |
waves.coherent_wave[:].profiles_2d[:].ion[:].element (alpha) | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
waves.coherent_wave[:].profiles_2d[:].ion[:].element[:].a (alpha) | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
waves.coherent_wave[:].profiles_2d[:].ion[:].element[:].multiplicity (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
waves.coherent_wave[:].profiles_2d[:].ion[:].element[:].z_n (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
waves.coherent_wave[:].profiles_2d[:].ion[:].label (alpha) | STR_0D | String identifying the species (e.g. H+, D+, T+, He+2, C+, D2, DT, CD4, ...) | ||
waves.coherent_wave[:].profiles_2d[:].ion[:].multiple_states_flag (alpha) | INT_0D | Multiple state calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure | ||
waves.coherent_wave[:].profiles_2d[:].ion[:].power_density_fast (alpha) | [1...N, | FLT_2D (uncertain) | W.m^-3 | Absorbed wave power density on the fast species |
waves.coherent_wave[:].profiles_2d[:].ion[:].power_density_fast_n_tor (alpha) | [1...N, | FLT_3D (uncertain) | W.m^-3 | Absorbed wave power density on the fast species, per toroidal mode number |
waves.coherent_wave[:].profiles_2d[:].ion[:].power_density_thermal (alpha) | [1...N, | FLT_2D (uncertain) | W.m^-3 | Absorbed wave power density on the thermal species |
waves.coherent_wave[:].profiles_2d[:].ion[:].power_density_thermal_n_tor (alpha) | [1...N, | FLT_3D (uncertain) | W.m^-3 | Absorbed wave power density on the thermal species, per toroidal mode number |
waves.coherent_wave[:].profiles_2d[:].ion[:].state (alpha) | [1...N_charge_states] | STRUCT_ARRAY | Collisional exchange with the various states of the ion species (ionisation, energy, excitation, ...) | |
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].electron_configuration (alpha) | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].label (alpha) | STR_0D | String identifying charge state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].power_density_fast (alpha) | [1...N, | FLT_2D (uncertain) | W.m^-3 | Absorbed wave power density on the fast species |
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].power_density_fast_n_tor (alpha) | [1...N, | FLT_3D (uncertain) | W.m^-3 | Absorbed wave power density on the fast species, per toroidal mode number |
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].power_density_thermal (alpha) | [1...N, | FLT_2D (uncertain) | W.m^-3 | Absorbed wave power density on the thermal species |
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].power_density_thermal_n_tor (alpha) | [1...N, | FLT_3D (uncertain) | W.m^-3 | Absorbed wave power density on the thermal species, per toroidal mode number |
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].vibrational_level (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].vibrational_mode (alpha) | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].z_max (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
waves.coherent_wave[:].profiles_2d[:].ion[:].state[:].z_min (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
waves.coherent_wave[:].profiles_2d[:].ion[:].z_ion (alpha) | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed). | |
waves.coherent_wave[:].profiles_2d[:].n_tor (alpha) | [1...N] | INT_1D | Toroidal mode numbers | |
waves.coherent_wave[:].profiles_2d[:].power_density (alpha) | [1...N, | FLT_2D (uncertain) | W.m^-3 | Total absorbed wave power density (electrons + ion + fast populations) |
waves.coherent_wave[:].profiles_2d[:].power_density_n_tor (alpha) | [1...N, | FLT_3D (uncertain) | W.m^-3 | Absorbed wave power density per toroidal mode number |
waves.coherent_wave[:].profiles_2d[:].time (alpha) | FLT_0D | s | Time | |
waves.coherent_wave[:].wave_solver_type (alpha) | STRUCTURE | Type of wave deposition solver used for this wave. Index = 1 for beam/ray tracing; index = 2 for full wave | ||
waves.coherent_wave[:].wave_solver_type.description (alpha) | STR_0D | Verbose description | ||
waves.coherent_wave[:].wave_solver_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list) | ||
waves.coherent_wave[:].wave_solver_type.name (alpha) | STR_0D | Short string identifier | ||
waves.ids_properties (alpha) | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
waves.ids_properties.comment (alpha) | STR_0D | Any comment describing the content of this IDS | ||
waves.ids_properties.homogeneous_time (alpha) | INT_0D | 1 if the time of this IDS is homogeneous. In this case, the time values for this IDS are stored in ../time just below the root of this IDS. Otherwise, the time values are stored in the various time fields at lower levels in the tree. | ||
waves.ids_properties.occurrence | INT_0D | |||
waves.magnetic_axis (alpha) | STRUCTURE | Magnetic axis position (used to define a poloidal angle for the 2D profiles) | ||
waves.magnetic_axis.r (alpha) | [waves.time] | FLT_1D (uncertain) | m | Major radius |
waves.magnetic_axis.z (alpha) | [waves.time] | FLT_1D (uncertain) | m | Height |
waves.time (alpha) | [1...N] | FLT_1D_TYPE | Generic time [s] | |
waves.vacuum_toroidal_field (alpha) | STRUCTURE | Characteristics of the vacuum toroidal field (used in rho_tor definition) | ||
waves.vacuum_toroidal_field.b0 (alpha) | [waves.time] | FLT_1D (uncertain) | T | Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewed from above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf IDS. |
waves.vacuum_toroidal_field.r0 (alpha) | FLT_0D (uncertain) | m | Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane) |