edge sources¶
Path | Dimensions | Type | Units | Description |
---|---|---|---|---|
edge_sources | 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 | STRUCTURE | Generic decription of the code-specific parameters for the code that has produced this IDS | ||
edge_sources.code.commit | STR_0D | Unique commit reference of software | ||
edge_sources.code.description | STR_0D | Short description of the software (type, purpose) | ||
edge_sources.code.library | [1...N] | STRUCT_ARRAY | List of external libraries used by the code that has produced this IDS | |
edge_sources.code.library[:].commit | STR_0D | Unique commit reference of software | ||
edge_sources.code.library[:].description | STR_0D | Short description of the software (type, purpose) | ||
edge_sources.code.library[:].name | STR_0D | Name of software | ||
edge_sources.code.library[:].parameters | STR_0D | List of the code specific parameters in XML format | ||
edge_sources.code.library[:].repository | STR_0D | URL of software repository | ||
edge_sources.code.library[:].version | STR_0D | Unique version (tag) of software | ||
edge_sources.code.name | STR_0D | Name of software generating IDS | ||
edge_sources.code.output_flag | [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 | STR_0D | List of the code specific parameters in XML format | ||
edge_sources.code.repository | STR_0D | URL of software repository | ||
edge_sources.code.version | STR_0D | Unique version (tag) of software | ||
edge_sources.grid_ggd | [edge_sources.grid_ggd[:].time] | STRUCT_ARRAY | Grid (using the Generic Grid Description), for various time slices. The timebase of this array of structure must be a subset of the ggd timebases | |
edge_sources.grid_ggd[:].grid_subset | [1...N] | STRUCT_ARRAY | Grid subsets | |
edge_sources.grid_ggd[:].grid_subset[:].base | [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.grid_ggd[:].grid_subset[:].base[:].jacobian | [edge_sources.grid_ggd[:].grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_sources.grid_ggd[:].grid_subset[:].base[:].tensor_contravariant | [edge_sources.grid_ggd[:].grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_sources.grid_ggd[:].grid_subset[:].base[:].tensor_covariant | [edge_sources.grid_ggd[:].grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_sources.grid_ggd[:].grid_subset[:].dimension | INT_0D | Space dimension of the grid subset elements, using the convention 1=nodes, 2=edges, 3=faces, 4=cells/volumes | ||
edge_sources.grid_ggd[:].grid_subset[:].element | [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.grid_ggd[:].grid_subset[:].element[:].object | [1...N] | STRUCT_ARRAY | Set of objects defining the element | |
edge_sources.grid_ggd[:].grid_subset[:].element[:].object[:].dimension | INT_0D | Dimension of the object - using the convention 1=nodes, 2=edges, 3=faces, 4=cells/volumes | ||
edge_sources.grid_ggd[:].grid_subset[:].element[:].object[:].index | INT_0D | Object index | ||
edge_sources.grid_ggd[:].grid_subset[:].element[:].object[:].space | INT_0D | Index of the space from which that object is taken | ||
edge_sources.grid_ggd[:].grid_subset[:].identifier | STRUCTURE | Grid subset identifier | ||
edge_sources.grid_ggd[:].grid_subset[:].identifier.description | STR_0D | Verbose description | ||
edge_sources.grid_ggd[:].grid_subset[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.grid_ggd[:].grid_subset[:].identifier.name | STR_0D | Short string identifier | ||
edge_sources.grid_ggd[:].grid_subset[:].metric | STRUCTURE | Metric of the canonical frame onto Cartesian coordinates | ||
edge_sources.grid_ggd[:].grid_subset[:].metric.jacobian | [edge_sources.grid_ggd[:].grid_subset[:].element] | FLT_1D (uncertain) | mixed | Metric Jacobian |
edge_sources.grid_ggd[:].grid_subset[:].metric.tensor_contravariant | [edge_sources.grid_ggd[:].grid_subset[:].element, | FLT_3D (uncertain) | mixed | Contravariant metric tensor, given on each element of the subgrid (first dimension) |
edge_sources.grid_ggd[:].grid_subset[:].metric.tensor_covariant | [edge_sources.grid_ggd[:].grid_subset[:].element, | FLT_3D (uncertain) | mixed | Covariant metric tensor, given on each element of the subgrid (first dimension) |
edge_sources.grid_ggd[:].identifier | STRUCTURE | Grid identifier | ||
edge_sources.grid_ggd[:].identifier.description | STR_0D | Verbose description | ||
edge_sources.grid_ggd[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.grid_ggd[:].identifier.name | STR_0D | Short string identifier | ||
edge_sources.grid_ggd[:].path | STR_0D | Path of the grid, including the IDS name, in case of implicit reference to a grid_ggd node described in another IDS. To be filled only if the grid is not described explicitly in this grid_ggd structure. Example syntax: IDS::wall/0/description_ggd(1)/grid_ggd, means that the grid is located in the wall IDS, occurrence 0, with relative path description_ggd(1)/grid_ggd, using Fortran index convention (here : first index of the array) | ||
edge_sources.grid_ggd[:].space | [1...N] | STRUCT_ARRAY | Set of grid spaces | |
edge_sources.grid_ggd[:].space[:].coordinates_type | [1...N] | INT_1D | Type of coordinates describing the physical space, for every coordinate of the space. The size of this node therefore defines the dimension of the space. The meaning of these predefined integer constants can be found in the Data Dictionary under utilities/coordinate_identifier.xml | |
edge_sources.grid_ggd[:].space[:].geometry_type | STRUCTURE | Type of space geometry (0: standard, 1:Fourier, >1: Fourier with periodicity) | ||
edge_sources.grid_ggd[:].space[:].geometry_type.description | STR_0D | Verbose description | ||
edge_sources.grid_ggd[:].space[:].geometry_type.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.grid_ggd[:].space[:].geometry_type.name | STR_0D | Short string identifier | ||
edge_sources.grid_ggd[:].space[:].identifier | STRUCTURE | Space identifier | ||
edge_sources.grid_ggd[:].space[:].identifier.description | STR_0D | Verbose description | ||
edge_sources.grid_ggd[:].space[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.grid_ggd[:].space[:].identifier.name | STR_0D | Short string identifier | ||
edge_sources.grid_ggd[:].space[:].objects_per_dimension | [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.grid_ggd[:].space[:].objects_per_dimension[:].geometry_content | STRUCTURE | Content of the ../object/geometry node for this dimension | ||
edge_sources.grid_ggd[:].space[:].objects_per_dimension[:].geometry_content.description | STR_0D | Verbose description | ||
edge_sources.grid_ggd[:].space[:].objects_per_dimension[:].geometry_content.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.grid_ggd[:].space[:].objects_per_dimension[:].geometry_content.name | STR_0D | Short string identifier | ||
edge_sources.grid_ggd[:].space[:].objects_per_dimension[:].object | [1...N] | STRUCT_ARRAY | Set of objects for a given dimension | |
edge_sources.grid_ggd[:].space[:].objects_per_dimension[:].object[:].boundary | [1...N] | STRUCT_ARRAY | Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object | |
edge_sources.grid_ggd[:].space[:].objects_per_dimension[:].object[:].boundary[:].index | INT_0D | Index of this (n-1)-dimensional boundary object | ||
edge_sources.grid_ggd[:].space[:].objects_per_dimension[:].object[:].boundary[:].neighbours | [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.grid_ggd[:].space[:].objects_per_dimension[:].object[:].geometry | [1...N] | FLT_1D (uncertain) | mixed | Geometry data associated with the object, its detailed content is defined by ../../geometry_content. Its dimension depends on the type of object, geometry and coordinate considered. |
edge_sources.grid_ggd[:].space[:].objects_per_dimension[:].object[:].geometry_2d | [1...N, | FLT_2D (uncertain) | mixed | 2D geometry data associated with the object. Its dimension depends on the type of object, geometry and coordinate considered. Typically, the first dimension represents the object coordinates, while the second dimension would represent the values of the various degrees of freedom of the finite element attached to the object. |
edge_sources.grid_ggd[:].space[:].objects_per_dimension[:].object[:].measure | 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.grid_ggd[:].space[:].objects_per_dimension[:].object[:].nodes | [1...N] | INT_1D | List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation) | |
edge_sources.grid_ggd[:].time | FLT_0D | s | Time | |
edge_sources.ids_properties | STRUCTURE | Interface Data Structure properties. This element identifies the node above as an IDS | ||
edge_sources.ids_properties.comment | STR_0D | Any comment describing the content of this IDS | ||
edge_sources.ids_properties.creation_date | STR_0D | Date at which this data has been produced | ||
edge_sources.ids_properties.homogeneous_time | INT_0D | This node must be filled (with 0, 1, or 2) for the IDS to be valid. If 1, the time of this IDS is homogeneous, i.e. the time values for this IDS are stored in the time node just below the root of this IDS. If 0, the time values are stored in the various time fields at lower levels in the tree. In the case only constant or static nodes are filled within the IDS, homogeneous_time must be set to 2 | ||
edge_sources.ids_properties.name | STR_0D | User-defined name for this IDS occurrence | ||
edge_sources.ids_properties.occurrence | INT_0D | |||
edge_sources.ids_properties.occurrence_type | STRUCTURE | Type of data contained in this occurrence | ||
edge_sources.ids_properties.occurrence_type.description | STR_0D | Verbose description | ||
edge_sources.ids_properties.occurrence_type.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.ids_properties.occurrence_type.name | STR_0D | Short string identifier | ||
edge_sources.ids_properties.plugins (alpha) | STRUCTURE | Information about the plugins used to write/read this IDS. This structure is filled automatically by the Access Layer at GET/PUT time, no need to fill it via a user program. | ||
edge_sources.ids_properties.plugins.infrastructure_get (alpha) | STRUCTURE | Plugin infrastructure used to GET the data | ||
edge_sources.ids_properties.plugins.infrastructure_get.commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_sources.ids_properties.plugins.infrastructure_get.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_sources.ids_properties.plugins.infrastructure_get.name (alpha) | STR_0D | Name of software used | ||
edge_sources.ids_properties.plugins.infrastructure_get.repository (alpha) | STR_0D | URL of software repository | ||
edge_sources.ids_properties.plugins.infrastructure_get.version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_sources.ids_properties.plugins.infrastructure_put (alpha) | STRUCTURE | Plugin infrastructure used to PUT the data | ||
edge_sources.ids_properties.plugins.infrastructure_put.commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_sources.ids_properties.plugins.infrastructure_put.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_sources.ids_properties.plugins.infrastructure_put.name (alpha) | STR_0D | Name of software used | ||
edge_sources.ids_properties.plugins.infrastructure_put.repository (alpha) | STR_0D | URL of software repository | ||
edge_sources.ids_properties.plugins.infrastructure_put.version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_sources.ids_properties.plugins.node (alpha) | [1...N] | STRUCT_ARRAY | Set of IDS nodes for which a plugin has been applied | |
edge_sources.ids_properties.plugins.node[:].get_operation (alpha) | [1...N] | STRUCT_ARRAY | Plugins actually used to read back a node (potentially, multiple plugins can be applied, listed in reverse order of application). This information is filled by the plugin infrastructure during the GET operation. | |
edge_sources.ids_properties.plugins.node[:].get_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_sources.ids_properties.plugins.node[:].get_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_sources.ids_properties.plugins.node[:].get_operation[:].name (alpha) | STR_0D | Name of software used | ||
edge_sources.ids_properties.plugins.node[:].get_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
edge_sources.ids_properties.plugins.node[:].get_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
edge_sources.ids_properties.plugins.node[:].get_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_sources.ids_properties.plugins.node[:].path (alpha) | STR_0D | Path of the node within the IDS, following the syntax given in the link below. If empty, means the plugin applies to the whole IDS. | ||
edge_sources.ids_properties.plugins.node[:].put_operation (alpha) | [1...N] | STRUCT_ARRAY | Plugins used to PUT a node (potentially, multiple plugins can be applied, if so they are listed by order of application) | |
edge_sources.ids_properties.plugins.node[:].put_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_sources.ids_properties.plugins.node[:].put_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_sources.ids_properties.plugins.node[:].put_operation[:].name (alpha) | STR_0D | Name of software used | ||
edge_sources.ids_properties.plugins.node[:].put_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
edge_sources.ids_properties.plugins.node[:].put_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
edge_sources.ids_properties.plugins.node[:].put_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_sources.ids_properties.plugins.node[:].readback (alpha) | [1...N] | STRUCT_ARRAY | Plugins to be used to read back a node (potentially, multiple plugins can be applied, listed in reverse order of application) | |
edge_sources.ids_properties.plugins.node[:].readback[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
edge_sources.ids_properties.plugins.node[:].readback[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
edge_sources.ids_properties.plugins.node[:].readback[:].name (alpha) | STR_0D | Name of software used | ||
edge_sources.ids_properties.plugins.node[:].readback[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
edge_sources.ids_properties.plugins.node[:].readback[:].repository (alpha) | STR_0D | URL of software repository | ||
edge_sources.ids_properties.plugins.node[:].readback[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
edge_sources.ids_properties.provenance (alpha) | STRUCTURE | Provenance information about this IDS | ||
edge_sources.ids_properties.provenance.node (alpha) | [1...N] | STRUCT_ARRAY | Set of IDS nodes for which the provenance is given. The provenance information applies to the whole structure below the IDS node. For documenting provenance information for the whole IDS, set the size of this array of structure to 1 and leave the child "path" node empty | |
edge_sources.ids_properties.provenance.node[:].path (alpha) | STR_0D | Path of the node within the IDS, following the syntax given in the link below. If empty, means the provenance information applies to the whole IDS. | ||
edge_sources.ids_properties.provenance.node[:].sources (alpha) | [1...N] | STR_1D | List of sources used to import or calculate this node, identified as explained below. In case the node is the result of of a calculation / data processing, the source is an input to the process described in the "code" structure at the root of the IDS. The source can be an IDS (identified by a URI or a persitent identifier, see syntax in the link below) or non-IDS data imported directly from an non-IMAS database (identified by the command used to import the source, or the persistent identifier of the data source). Often data are obtained by a chain of processes, however only the last process input are recorded here. The full chain of provenance has then to be reconstructed recursively from the provenance information contained in the data sources. | |
edge_sources.ids_properties.provider | STR_0D | Name of the person in charge of producing this data | ||
edge_sources.ids_properties.source (obsolescent) | STR_0D | Source of the data (any comment describing the origin of the data : code, path to diagnostic signals, processing method, ...). Superseeded by the new provenance structure. | ||
edge_sources.ids_properties.version_put | STRUCTURE | Version of the access layer package used to PUT this IDS | ||
edge_sources.ids_properties.version_put.access_layer | STR_0D | Version of Access Layer used to PUT this IDS | ||
edge_sources.ids_properties.version_put.access_layer_language | STR_0D | Programming language of the Access Layer high level API used to PUT this IDS | ||
edge_sources.ids_properties.version_put.data_dictionary | STR_0D | Version of Data Dictionary used to PUT this IDS | ||
edge_sources.midplane | STRUCTURE | Choice of midplane definition (use the lowest index number if more than one value is relevant) | ||
edge_sources.midplane.description | STR_0D | Verbose description | ||
edge_sources.midplane.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.midplane.name | STR_0D | Short string identifier | ||
edge_sources.source | [1...N] | STRUCT_ARRAY | Set of source terms | |
edge_sources.source[:].ggd | [edge_sources.source[:].ggd[:].time] | STRUCT_ARRAY | Source terms represented using the general grid description, for various time slices | |
edge_sources.source[:].ggd[:].current | [1...N] | STRUCT_ARRAY | A.m^-2 | Current density source |
edge_sources.source[:].ggd[:].current[:].coefficients | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].current[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].current[:].values | [1...N] | FLT_1D (uncertain) | A.m^-2 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].electrons | STRUCTURE | Sources for electrons | ||
edge_sources.source[:].ggd[:].electrons.energy | [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 | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].electrons.energy[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].electrons.energy[:].values | [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 | [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 | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].electrons.particles[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].electrons.particles[:].values | [1...N] | FLT_1D (uncertain) | m^-3.s^-1 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion | [1...N] | STRUCT_ARRAY | Source terms related to the different ion species, in the sense of isonuclear or isomolecular sequences. Ionisation states (and other types of states) must be differentiated at the state level below | |
edge_sources.source[:].ggd[:].ion[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_sources.source[:].ggd[:].ion[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_sources.source[:].ggd[:].ion[:].element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_sources.source[:].ggd[:].ion[:].element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_sources.source[:].ggd[:].ion[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_sources.source[:].ggd[:].ion[:].energy | [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 | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].energy[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].ion[:].energy[:].values | [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 | STR_0D | String identifying ion (e.g. H, D, T, He, C, D2, ...) | ||
edge_sources.source[:].ggd[:].ion[:].momentum | [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 | [1...N] | 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 | [1...N, | 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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].momentum[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].ion[:].momentum[:].parallel | [1...N] | 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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].r | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].momentum[:].r_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the major radius axis, to 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 | [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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].momentum[:].z | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].momentum[:].z_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the height axis, to 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 | INT_0D | Multiple states calculation flag : 0-Only the 'ion' level is considered and the 'state' array of structure is empty; 1-Ion states are considered and are described in the 'state' array of structure | ||
edge_sources.source[:].ggd[:].ion[:].neutral_index | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
edge_sources.source[:].ggd[:].ion[:].particles | [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 | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].particles[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].ion[:].particles[:].values | [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 | [1...N] | STRUCT_ARRAY | Source terms related to the different states of the species (ionisation, energy, excitation, ...) | |
edge_sources.source[:].ggd[:].ion[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_sources.source[:].ggd[:].ion[:].state[:].energy | [1...N] | STRUCT_ARRAY | W.m^-3 | Source terms for the state energy transport equation |
edge_sources.source[:].ggd[:].ion[:].state[:].energy[:].coefficients | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].state[:].energy[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].ion[:].state[:].energy[:].values | [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 | STR_0D | String identifying state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
edge_sources.source[:].ggd[:].ion[:].state[:].momentum | [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 | [1...N] | 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 | [1...N, | 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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].parallel | [1...N] | 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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].r | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].r_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the major radius axis, to 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 | [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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].momentum[:].z | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].ion[:].state[:].momentum[:].z_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the height axis, to 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 | [1...N] | STRUCT_ARRAY | s^-1.m^-3 | Source term for the state density transport equation |
edge_sources.source[:].ggd[:].ion[:].state[:].particles[:].coefficients | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].ion[:].state[:].particles[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].ion[:].state[:].particles[:].values | [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 | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_sources.source[:].ggd[:].ion[:].state[:].vibrational_mode | 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 | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the state bundle | |
edge_sources.source[:].ggd[:].ion[:].state[:].z_min | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the state bundle | |
edge_sources.source[:].ggd[:].ion[:].z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
edge_sources.source[:].ggd[:].momentum | [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 | [1...N] | 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 | [1...N, | 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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].momentum[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].momentum[:].parallel | [1...N] | 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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].r | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].momentum[:].r_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the major radius axis, to 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 | [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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].momentum[:].z | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].momentum[:].z_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the height axis, to 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 | [1...N] | STRUCT_ARRAY | Source terms related to the different neutral species | |
edge_sources.source[:].ggd[:].neutral[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_sources.source[:].ggd[:].neutral[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_sources.source[:].ggd[:].neutral[:].element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_sources.source[:].ggd[:].neutral[:].element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_sources.source[:].ggd[:].neutral[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_sources.source[:].ggd[:].neutral[:].energy | [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 | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].energy[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].neutral[:].energy[:].values | [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 | INT_0D | Index of the corresponding ion species in the ../../ion array | ||
edge_sources.source[:].ggd[:].neutral[:].label | STR_0D | String identifying neutral (e.g. H, D, T, He, C, ...) | ||
edge_sources.source[:].ggd[:].neutral[:].momentum | [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 | [1...N] | 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 | [1...N, | 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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].momentum[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].neutral[:].momentum[:].parallel | [1...N] | 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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].r | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].r_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the major radius axis, to 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 | [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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].momentum[:].z | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].momentum[:].z_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the height axis, to 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 | 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 | [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 | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].particles[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].neutral[:].particles[:].values | [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 | [1...N] | STRUCT_ARRAY | Source terms related to the different states of the species (energy, excitation, ...) | |
edge_sources.source[:].ggd[:].neutral[:].state[:].electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].energy | [1...N] | STRUCT_ARRAY | W.m^-3 | Source terms for the state energy transport equation |
edge_sources.source[:].ggd[:].neutral[:].state[:].energy[:].coefficients | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].energy[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].energy[:].values | [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 | STR_0D | String identifying state | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum | [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 | [1...N] | 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 | [1...N, | 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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].parallel | [1...N] | 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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].r | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the major radius axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].r_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the major radius axis, to 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 | [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 | [1...N, | 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 | [1...N] | 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 | [1...N, | 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[:].momentum[:].z | [1...N] | FLT_1D (uncertain) | kg.m^-1.s^-2 | Component along the height axis, one scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd[:].neutral[:].state[:].momentum[:].z_coefficients | [1...N, | FLT_2D (uncertain) | kg.m^-1.s^-2 | Interpolation coefficients for the component along the height axis, to 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 | 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 | STR_0D | Verbose description | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].neutral_type.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].neutral_type.name | STR_0D | Short string identifier | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].particles | [1...N] | STRUCT_ARRAY | s^-1.m^-3 | Source term for the state density transport equation |
edge_sources.source[:].ggd[:].neutral[:].state[:].particles[:].coefficients | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].particles[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].neutral[:].state[:].particles[:].values | [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 | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_sources.source[:].ggd[:].neutral[:].state[:].vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_sources.source[:].ggd[:].time | FLT_0D | s | Time | |
edge_sources.source[:].ggd[:].total_ion_energy | [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 | [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 | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd[:].total_ion_energy[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd[:].total_ion_energy[:].values | [1...N] | FLT_1D (uncertain) | W.m^-3 | One scalar value is provided per element in the grid subset. |
edge_sources.source[:].ggd_fast | [edge_sources.source[:].ggd_fast[:].time] | STRUCT_ARRAY | Quantities provided at a faster sampling rate than the full ggd quantities. These are either integrated quantities or local quantities provided on a reduced set of positions. Positions and integration domains are described by a set of grid_subsets (of size 1 for a position). | |
edge_sources.source[:].ggd_fast[:].ion | [1...N] | STRUCT_ARRAY | Source term integrals related to the various ion species | |
edge_sources.source[:].ggd_fast[:].ion[:].element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_sources.source[:].ggd_fast[:].ion[:].element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_sources.source[:].ggd_fast[:].ion[:].element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_sources.source[:].ggd_fast[:].ion[:].element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_sources.source[:].ggd_fast[:].ion[:].element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_sources.source[:].ggd_fast[:].ion[:].label | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
edge_sources.source[:].ggd_fast[:].ion[:].neutral_index | INT_0D | Index of the corresponding neutral species in the ../../neutral array | ||
edge_sources.source[:].ggd_fast[:].ion[:].power | [1...N] | STRUCT_ARRAY | W | Total power source or sink related to this ion species, integrated over the volume of the grid subset, for various grid subsets. |
edge_sources.source[:].ggd_fast[:].ion[:].power[:].grid_index | INT_0D | Index of the grid used to represent this quantity | ||
edge_sources.source[:].ggd_fast[:].ion[:].power[:].grid_subset_index | INT_0D | Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index | ||
edge_sources.source[:].ggd_fast[:].ion[:].power[:].value | FLT_0D (uncertain) | W | Scalar value of the quantity on the grid subset (corresponding to a single local position or to an integrated value over the subset) | |
edge_sources.source[:].ggd_fast[:].ion[:].z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
edge_sources.source[:].ggd_fast[:].time | FLT_0D | s | Time | |
edge_sources.source[:].identifier | STRUCTURE | Source term identifier (process causing this source term) | ||
edge_sources.source[:].identifier.description | STR_0D | Verbose description | ||
edge_sources.source[:].identifier.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.source[:].identifier.name | STR_0D | Short string identifier | ||
edge_sources.source[:].species | STRUCTURE | Species causing this source term (if relevant, e.g. a particular ion or neutral state in case of line radiation) | ||
edge_sources.source[:].species.ion | STRUCTURE | Description of the ion or neutral species, used if type/index = 2 or 3 | ||
edge_sources.source[:].species.ion.element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_sources.source[:].species.ion.element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_sources.source[:].species.ion.element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_sources.source[:].species.ion.element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_sources.source[:].species.ion.element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_sources.source[:].species.ion.label | STR_0D | String identifying ion (e.g. H+, D+, T+, He+2, C+, ...) | ||
edge_sources.source[:].species.ion.state | STRUCTURE | Quantities related to the different states of the species (ionisation, energy, excitation, ...) | ||
edge_sources.source[:].species.ion.state.electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_sources.source[:].species.ion.state.label | STR_0D | String identifying ion state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, ...) | ||
edge_sources.source[:].species.ion.state.vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_sources.source[:].species.ion.state.vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_sources.source[:].species.ion.state.z_max | FLT_0D (uncertain) | Elementary Charge Unit | Maximum Z of the charge state bundle (equal to z_min if no bundle) | |
edge_sources.source[:].species.ion.state.z_min | FLT_0D (uncertain) | Elementary Charge Unit | Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral) | |
edge_sources.source[:].species.ion.z_ion | FLT_0D (uncertain) | Elementary Charge Unit | Ion charge (of the dominant ionisation state; lumped ions are allowed) | |
edge_sources.source[:].species.neutral | STRUCTURE | Description of the neutral species, used if type/index = 4 or 5 | ||
edge_sources.source[:].species.neutral.element | [1...N] | STRUCT_ARRAY | List of elements forming the atom or molecule | |
edge_sources.source[:].species.neutral.element[:].a | FLT_0D (uncertain) | Atomic Mass Unit | Mass of atom | |
edge_sources.source[:].species.neutral.element[:].atoms_n | INT_0D | Number of atoms of this element in the molecule | ||
edge_sources.source[:].species.neutral.element[:].multiplicity (obsolescent) | FLT_0D (uncertain) | Elementary Charge Unit | Multiplicity of the atom | |
edge_sources.source[:].species.neutral.element[:].z_n | FLT_0D (uncertain) | Elementary Charge Unit | Nuclear charge | |
edge_sources.source[:].species.neutral.label | STR_0D | String identifying neutral (e.g. H, D, T, He, C, ...) | ||
edge_sources.source[:].species.neutral.state | STRUCTURE | State of the species (energy, excitation, ...) | ||
edge_sources.source[:].species.neutral.state.electron_configuration | STR_0D | Configuration of atomic orbitals of this state, e.g. 1s2-2s1 | ||
edge_sources.source[:].species.neutral.state.label | STR_0D | String identifying neutral state | ||
edge_sources.source[:].species.neutral.state.neutral_type | STRUCTURE | Neutral type, in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI | ||
edge_sources.source[:].species.neutral.state.neutral_type.description | STR_0D | Verbose description | ||
edge_sources.source[:].species.neutral.state.neutral_type.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.source[:].species.neutral.state.neutral_type.name | STR_0D | Short string identifier | ||
edge_sources.source[:].species.neutral.state.vibrational_level | FLT_0D (uncertain) | Elementary Charge Unit | Vibrational level (can be bundled) | |
edge_sources.source[:].species.neutral.state.vibrational_mode | STR_0D | Vibrational mode of this state, e.g. "A_g". Need to define, or adopt a standard nomenclature. | ||
edge_sources.source[:].species.type | 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 | ||
edge_sources.source[:].species.type.description | STR_0D | Verbose description | ||
edge_sources.source[:].species.type.index | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
edge_sources.source[:].species.type.name | STR_0D | Short string identifier | ||
edge_sources.time | [1...N] | FLT_1D_TYPE | s | Generic time |