transport solver numerics¶
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 solver_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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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) | 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). Private identifier values must be indicated by a negative index. | ||
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). Private identifier values must be indicated by a negative index. | ||
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) | 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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | STRUCTURE | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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). Private identifier values must be indicated by a negative index. | ||
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, using the convention 1=nodes, 2=edges, 3=faces, 4=cells/volumes | ||
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 - using the convention 1=nodes, 2=edges, 3=faces, 4=cells/volumes | ||
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). Private identifier values must be indicated by a negative index. | ||
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). Private identifier values must be indicated by a negative index. | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.path (alpha) | 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: 'wall:0/description_ggd(1)/grid_ggd', means that the grid is located in the wall IDS, occurrence 0, with ids path 'description_ggd(1)/grid_ggd'. See the link below for more details about IDS paths | ||
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 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 | |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].geometry_type (alpha) | STRUCTURE | Type of space geometry (0: standard, 1:Fourier, >1: Fourier with periodicity) | ||
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). Private identifier values must be indicated by a negative index. | ||
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[:].identifier (alpha) | STRUCTURE | Space identifier | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].identifier.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[:].geometry_content (alpha) | STRUCTURE | Content of the ../object/geometry node for this dimension | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].geometry_content.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].geometry_content.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].geometry_content.name (alpha) | STR_0D | Short string identifier | ||
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 detailed content is defined by ../../geometry_content. Its dimension depends on the type of object, geometry and coordinate considered. |
transport_solver_numerics.boundary_conditions_ggd[:].grid.space[:].objects_per_dimension[:].object[:].geometry_2d (alpha) | [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. |
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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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). Private identifier values must be indicated by a negative index. | ||
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) | 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). Private identifier values must be indicated by a negative index. | ||
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). Private identifier values must be indicated by a negative index. | ||
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) | 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). Private identifier values must be indicated by a negative index. | ||
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.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
transport_solver_numerics.code.library (alpha) | [1...N] | STRUCT_ARRAY | List of external libraries used by the code that has produced this IDS | |
transport_solver_numerics.code.library[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
transport_solver_numerics.code.library[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
transport_solver_numerics.code.library[:].name (alpha) | STR_0D | Name of software | ||
transport_solver_numerics.code.library[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
transport_solver_numerics.code.library[:].repository (alpha) | STR_0D | URL of software repository | ||
transport_solver_numerics.code.library[:].version (alpha) | STR_0D | Unique version (tag) 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 To be removed when the solver_1d structure is finalized. | ||
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.delta_relative (alpha) | STRUCTURE | Relative deviation on the primary quantity of the transport equation between the present and the previous iteration of the solver | ||
transport_solver_numerics.convergence.equations[:].current.delta_relative.expression (alpha) | STR_0D | Expression used by the solver to calculate the relative deviation | ||
transport_solver_numerics.convergence.equations[:].current.delta_relative.value (alpha) | FLT_0D (uncertain) | - | Value of the relative deviation | |
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) | STRUCTURE | W.m^-3 | Convergence details of the electron energy equation | |
transport_solver_numerics.convergence.equations[:].electrons.energy.delta_relative (alpha) | STRUCTURE | Relative deviation on the primary quantity of the transport equation between the present and the previous iteration of the solver | ||
transport_solver_numerics.convergence.equations[:].electrons.energy.delta_relative.expression (alpha) | STR_0D | Expression used by the solver to calculate the relative deviation | ||
transport_solver_numerics.convergence.equations[:].electrons.energy.delta_relative.value (alpha) | FLT_0D (uncertain) | - | Value of the relative deviation | |
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) | STRUCTURE | m^-3.s^-1 | Convergence details of the electron density equation | |
transport_solver_numerics.convergence.equations[:].electrons.particles.delta_relative (alpha) | STRUCTURE | Relative deviation on the primary quantity of the transport equation between the present and the previous iteration of the solver | ||
transport_solver_numerics.convergence.equations[:].electrons.particles.delta_relative.expression (alpha) | STR_0D | Expression used by the solver to calculate the relative deviation | ||
transport_solver_numerics.convergence.equations[:].electrons.particles.delta_relative.value (alpha) | FLT_0D (uncertain) | - | Value of the relative deviation | |
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) | STRUCTURE | W.m^-3 | Convergence details of the ion total (sum over ion species) energy equation | |
transport_solver_numerics.convergence.equations[:].energy_ion_total.delta_relative (alpha) | STRUCTURE | Relative deviation on the primary quantity of the transport equation between the present and the previous iteration of the solver | ||
transport_solver_numerics.convergence.equations[:].energy_ion_total.delta_relative.expression (alpha) | STR_0D | Expression used by the solver to calculate the relative deviation | ||
transport_solver_numerics.convergence.equations[:].energy_ion_total.delta_relative.value (alpha) | FLT_0D (uncertain) | - | Value of the relative deviation | |
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) | STRUCTURE | W.m^-3 | Convergence details of the ion energy equation | |
transport_solver_numerics.convergence.equations[:].ion[:].energy.delta_relative (alpha) | STRUCTURE | Relative deviation on the primary quantity of the transport equation between the present and the previous iteration of the solver | ||
transport_solver_numerics.convergence.equations[:].ion[:].energy.delta_relative.expression (alpha) | STR_0D | Expression used by the solver to calculate the relative deviation | ||
transport_solver_numerics.convergence.equations[:].ion[:].energy.delta_relative.value (alpha) | FLT_0D (uncertain) | - | Value of the relative deviation | |
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) | STRUCTURE | m^-3.s^-1 | Convergence details of the ion density equation | |
transport_solver_numerics.convergence.equations[:].ion[:].particles.delta_relative (alpha) | STRUCTURE | Relative deviation on the primary quantity of the transport equation between the present and the previous iteration of the solver | ||
transport_solver_numerics.convergence.equations[:].ion[:].particles.delta_relative.expression (alpha) | STR_0D | Expression used by the solver to calculate the relative deviation | ||
transport_solver_numerics.convergence.equations[:].ion[:].particles.delta_relative.value (alpha) | FLT_0D (uncertain) | - | Value of the relative deviation | |
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) | STRUCTURE | W.m^-3 | Convergence details of the charge state energy equation | |
transport_solver_numerics.convergence.equations[:].ion[:].state[:].energy.delta_relative (alpha) | STRUCTURE | Relative deviation on the primary quantity of the transport equation between the present and the previous iteration of the solver | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].energy.delta_relative.expression (alpha) | STR_0D | Expression used by the solver to calculate the relative deviation | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].energy.delta_relative.value (alpha) | FLT_0D (uncertain) | - | Value of the relative deviation | |
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). Private identifier values must be indicated by a negative index. | ||
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) | STRUCTURE | m^-3.s^-1 | Convergence details of the charge state density equation | |
transport_solver_numerics.convergence.equations[:].ion[:].state[:].particles.delta_relative (alpha) | STRUCTURE | Relative deviation on the primary quantity of the transport equation between the present and the previous iteration of the solver | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].particles.delta_relative.expression (alpha) | STR_0D | Expression used by the solver to calculate the relative deviation | ||
transport_solver_numerics.convergence.equations[:].ion[:].state[:].particles.delta_relative.value (alpha) | FLT_0D (uncertain) | - | Value of the relative deviation | |
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 | 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.data (alpha) | [transport_solver_numerics.convergence.time_step.time] | FLT_1D (uncertain) | s | Data |
transport_solver_numerics.convergence.time_step.time (alpha) | [1...N] | FLT_1D_TYPE | s | Time |
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 solver_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.psi_boundary (alpha) | FLT_0D (uncertain) | Wb | Value of the poloidal magnetic flux at the plasma boundary (useful to normalize the psi array values when the radial grid doesn't go from the magnetic axis to the plasma boundary) | |
transport_solver_numerics.derivatives_1d[:].grid.psi_magnetic_axis (alpha) | FLT_0D (uncertain) | Wb | Value of the poloidal magnetic flux at the magnetic axis (useful to normalize the psi array values when the radial grid doesn't go from the magnetic axis to the plasma boundary) | |
transport_solver_numerics.derivatives_1d[:].grid.rho_pol_norm (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate = sqrt((psi(rho)-psi(magnetic_axis)) / (psi(LCFS)-psi(magnetic_axis))) |
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.surface (alpha) | [transport_solver_numerics.derivatives_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Surface area of the toroidal flux surface |
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] | 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). Private identifier values must be indicated by a negative index. | ||
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.creation_date (alpha) | STR_0D | Date at which this data has been produced | ||
transport_solver_numerics.ids_properties.homogeneous_time (alpha) | 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 | ||
transport_solver_numerics.ids_properties.name (alpha) | STR_0D | User-defined name for this IDS occurrence | ||
transport_solver_numerics.ids_properties.occurrence | INT_0D | |||
transport_solver_numerics.ids_properties.occurrence_type (alpha) | STRUCTURE | Type of data contained in this occurrence | ||
transport_solver_numerics.ids_properties.occurrence_type.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.ids_properties.occurrence_type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
transport_solver_numerics.ids_properties.occurrence_type.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.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. | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_get (alpha) | STRUCTURE | Plugin infrastructure used to GET the data | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_get.commit (alpha) | STR_0D | Unique commit reference of software | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_get.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_get.name (alpha) | STR_0D | Name of software used | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_get.repository (alpha) | STR_0D | URL of software repository | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_get.version (alpha) | STR_0D | Unique version (tag) of software | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_put (alpha) | STRUCTURE | Plugin infrastructure used to PUT the data | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_put.commit (alpha) | STR_0D | Unique commit reference of software | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_put.description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_put.name (alpha) | STR_0D | Name of software used | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_put.repository (alpha) | STR_0D | URL of software repository | ||
transport_solver_numerics.ids_properties.plugins.infrastructure_put.version (alpha) | STR_0D | Unique version (tag) of software | ||
transport_solver_numerics.ids_properties.plugins.node (alpha) | [1...N] | STRUCT_ARRAY | Set of IDS nodes for which a plugin has been applied | |
transport_solver_numerics.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. | |
transport_solver_numerics.ids_properties.plugins.node[:].get_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
transport_solver_numerics.ids_properties.plugins.node[:].get_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
transport_solver_numerics.ids_properties.plugins.node[:].get_operation[:].name (alpha) | STR_0D | Name of software used | ||
transport_solver_numerics.ids_properties.plugins.node[:].get_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
transport_solver_numerics.ids_properties.plugins.node[:].get_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
transport_solver_numerics.ids_properties.plugins.node[:].get_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
transport_solver_numerics.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. | ||
transport_solver_numerics.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) | |
transport_solver_numerics.ids_properties.plugins.node[:].put_operation[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
transport_solver_numerics.ids_properties.plugins.node[:].put_operation[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
transport_solver_numerics.ids_properties.plugins.node[:].put_operation[:].name (alpha) | STR_0D | Name of software used | ||
transport_solver_numerics.ids_properties.plugins.node[:].put_operation[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
transport_solver_numerics.ids_properties.plugins.node[:].put_operation[:].repository (alpha) | STR_0D | URL of software repository | ||
transport_solver_numerics.ids_properties.plugins.node[:].put_operation[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
transport_solver_numerics.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) | |
transport_solver_numerics.ids_properties.plugins.node[:].readback[:].commit (alpha) | STR_0D | Unique commit reference of software | ||
transport_solver_numerics.ids_properties.plugins.node[:].readback[:].description (alpha) | STR_0D | Short description of the software (type, purpose) | ||
transport_solver_numerics.ids_properties.plugins.node[:].readback[:].name (alpha) | STR_0D | Name of software used | ||
transport_solver_numerics.ids_properties.plugins.node[:].readback[:].parameters (alpha) | STR_0D | List of the code specific parameters in XML format | ||
transport_solver_numerics.ids_properties.plugins.node[:].readback[:].repository (alpha) | STR_0D | URL of software repository | ||
transport_solver_numerics.ids_properties.plugins.node[:].readback[:].version (alpha) | STR_0D | Unique version (tag) of software | ||
transport_solver_numerics.ids_properties.provenance (alpha) | STRUCTURE | Provenance information about this IDS | ||
transport_solver_numerics.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 | |
transport_solver_numerics.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. | ||
transport_solver_numerics.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. | |
transport_solver_numerics.ids_properties.provider (alpha) | STR_0D | Name of the person in charge of producing this data | ||
transport_solver_numerics.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. | ||
transport_solver_numerics.ids_properties.version_put (alpha) | STRUCTURE | Version of the access layer package used to PUT this IDS | ||
transport_solver_numerics.ids_properties.version_put.access_layer (alpha) | STR_0D | Version of Access Layer used to PUT this IDS | ||
transport_solver_numerics.ids_properties.version_put.access_layer_language (alpha) | STR_0D | Programming language of the Access Layer high level API used to PUT this IDS | ||
transport_solver_numerics.ids_properties.version_put.data_dictionary (alpha) | STR_0D | Version of Data Dictionary used to PUT this IDS | ||
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). Private identifier values must be indicated by a negative index. | ||
transport_solver_numerics.primary_coordinate.name (alpha) | STR_0D | Short string identifier | ||
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). Private identifier values must be indicated by a negative index. | ||
transport_solver_numerics.solver.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.solver_1d (alpha) | [transport_solver_numerics.solver_1d[:].time] | STRUCT_ARRAY | Numerics related to 1D radial solver, for various time slices. | |
transport_solver_numerics.solver_1d[:].control_parameters (alpha) | STRUCTURE | Solver-specific input or output quantities | ||
transport_solver_numerics.solver_1d[:].control_parameters.integer0d (alpha) | [1...N] | STRUCT_ARRAY | Set of integer type scalar control parameters | |
transport_solver_numerics.solver_1d[:].control_parameters.integer0d[:].name (alpha) | STR_0D | Name of the control parameter | ||
transport_solver_numerics.solver_1d[:].control_parameters.integer0d[:].value (alpha) | INT_0D | Value of the control parameter | ||
transport_solver_numerics.solver_1d[:].control_parameters.real0d (alpha) | [1...N] | STRUCT_ARRAY | Set of real type scalar control parameters | |
transport_solver_numerics.solver_1d[:].control_parameters.real0d[:].name (alpha) | STR_0D | Name of the control parameter | ||
transport_solver_numerics.solver_1d[:].control_parameters.real0d[:].value (alpha) | FLT_0D (uncertain) | mixed | Value of the control parameter | |
transport_solver_numerics.solver_1d[:].d_dvolume_drho_tor_dt (alpha) | [transport_solver_numerics.solver_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.solver_1d[:].drho_tor_dt (alpha) | [transport_solver_numerics.solver_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.solver_1d[:].equation (alpha) | [1...N] | STRUCT_ARRAY | Set of transport equations | |
transport_solver_numerics.solver_1d[:].equation[:].boundary_condition (alpha) | [1...N] | STRUCT_ARRAY | Set of boundary conditions of the transport equation | |
transport_solver_numerics.solver_1d[:].equation[:].boundary_condition[:].position (alpha) | FLT_0D (uncertain) | mixed | Position, in terms of the primary coordinate, at which the boundary condition is imposed. Outside this position, the value of the data are considered to be prescribed (in case of a single boundary condition). | |
transport_solver_numerics.solver_1d[:].equation[:].boundary_condition[:].type (alpha) | STRUCTURE | Boundary condition type | ||
transport_solver_numerics.solver_1d[:].equation[:].boundary_condition[:].type.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.solver_1d[:].equation[:].boundary_condition[:].type.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
transport_solver_numerics.solver_1d[:].equation[:].boundary_condition[:].type.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.solver_1d[:].equation[:].boundary_condition[:].value (alpha) | [1...3] | FLT_1D (uncertain) | mixed | Value of the boundary condition. For type/index = 1 to 3, only the first position in the vector is used. For type/index = 5, all three positions are used, meaning respectively a1, a2, a3. |
transport_solver_numerics.solver_1d[:].equation[:].coefficient (alpha) | [1...N] | STRUCT_ARRAY | Set of numerical coefficients involved in the transport equation | |
transport_solver_numerics.solver_1d[:].equation[:].coefficient[:].profile (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Radial profile of the numerical coefficient |
transport_solver_numerics.solver_1d[:].equation[:].computation_mode (alpha) | STRUCTURE | Computation mode for this equation | ||
transport_solver_numerics.solver_1d[:].equation[:].computation_mode.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.solver_1d[:].equation[:].computation_mode.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
transport_solver_numerics.solver_1d[:].equation[:].computation_mode.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.solver_1d[:].equation[:].convergence (alpha) | STRUCTURE | Convergence details | ||
transport_solver_numerics.solver_1d[:].equation[:].convergence.delta_relative (alpha) | STRUCTURE | Relative deviation on the primary quantity of the transport equation between the present and the previous iteration of the solver | ||
transport_solver_numerics.solver_1d[:].equation[:].convergence.delta_relative.expression (alpha) | STR_0D | Expression used by the solver to calculate the relative deviation | ||
transport_solver_numerics.solver_1d[:].equation[:].convergence.delta_relative.value (alpha) | FLT_0D (uncertain) | - | Value of the relative deviation | |
transport_solver_numerics.solver_1d[:].equation[:].convergence.iterations_n (alpha) | INT_0D | Number of iterations carried out in the convergence loop | ||
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity (alpha) | STRUCTURE | Profile and derivatives of the primary quantity of the transport equation | ||
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.d2_dr2 (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Second order radial derivative with respect to the primary coordinate |
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.d_dr (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Radial derivative with respect to the primary coordinate |
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.d_dt (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Time derivative |
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.d_dt_cphi (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to time, at constant toroidal flux (for current diffusion equation) |
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.d_dt_cr (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Derivative with respect to time, at constant primary coordinate coordinate (for current diffusion equation) |
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.identifier (alpha) | STRUCTURE | Identifier of the primary quantity of the transport equation. The description node contains the path to the quantity in the physics IDS (example: core_profiles/profiles_1d/ion(1)/density) | ||
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.identifier.description (alpha) | STR_0D | Verbose description | ||
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.identifier.index (alpha) | INT_0D | Integer identifier (enumeration index within a list). Private identifier values must be indicated by a negative index. | ||
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.identifier.name (alpha) | STR_0D | Short string identifier | ||
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.ion_index (alpha) | INT_0D | If the primary quantity is related to a ion species, index of the corresponding species in the core_profiles/profiles_1d/ion array | ||
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.neutral_index (alpha) | INT_0D | If the primary quantity is related to a neutral species, index of the corresponding species in the core_profiles/profiles_1d/neutral array | ||
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.profile (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | mixed | Profile of the primary quantity |
transport_solver_numerics.solver_1d[:].equation[:].primary_quantity.state_index (alpha) | INT_0D | If the primary quantity is related to a particular state (of an ion or a neutral species), index of the corresponding state in the core_profiles/profiles_1d/ion (or neutral)/state array | ||
transport_solver_numerics.solver_1d[:].grid (alpha) | STRUCTURE | Radial grid | ||
transport_solver_numerics.solver_1d[:].grid.area (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Cross-sectional area of the flux surface |
transport_solver_numerics.solver_1d[:].grid.psi (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | Wb | Poloidal magnetic flux |
transport_solver_numerics.solver_1d[:].grid.psi_boundary (alpha) | FLT_0D (uncertain) | Wb | Value of the poloidal magnetic flux at the plasma boundary (useful to normalize the psi array values when the radial grid doesn't go from the magnetic axis to the plasma boundary) | |
transport_solver_numerics.solver_1d[:].grid.psi_magnetic_axis (alpha) | FLT_0D (uncertain) | Wb | Value of the poloidal magnetic flux at the magnetic axis (useful to normalize the psi array values when the radial grid doesn't go from the magnetic axis to the plasma boundary) | |
transport_solver_numerics.solver_1d[:].grid.rho_pol_norm (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | - | Normalised poloidal flux coordinate = sqrt((psi(rho)-psi(magnetic_axis)) / (psi(LCFS)-psi(magnetic_axis))) |
transport_solver_numerics.solver_1d[:].grid.rho_tor (alpha) | [transport_solver_numerics.solver_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.solver_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.solver_1d[:].grid.surface (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^2 | Surface area of the toroidal flux surface |
transport_solver_numerics.solver_1d[:].grid.volume (alpha) | [transport_solver_numerics.solver_1d[:].grid.rho_tor_norm] | FLT_1D (uncertain) | m^3 | Volume enclosed inside the magnetic surface |
transport_solver_numerics.solver_1d[:].time (alpha) | FLT_0D | s | Time | |
transport_solver_numerics.time (alpha) | [1...N] | FLT_1D_TYPE | s | Generic time |
transport_solver_numerics.time_step (alpha) | STRUCTURE | s | Internal time step used by the transport solver (assuming all transport equations are solved with the same time step) | |
transport_solver_numerics.time_step.data (alpha) | [transport_solver_numerics.time_step.time] | FLT_1D (uncertain) | s | Data |
transport_solver_numerics.time_step.time (alpha) | [1...N] | FLT_1D_TYPE | s | Time |
transport_solver_numerics.time_step_average (alpha) | STRUCTURE | s | Average internal time step used by the transport solver between the previous and the current time stored for this quantity (assuming all transport equations are solved with the same time step) | |
transport_solver_numerics.time_step_average.data (alpha) | [transport_solver_numerics.time_step_average.time] | FLT_1D (uncertain) | s | Data |
transport_solver_numerics.time_step_average.time (alpha) | [1...N] | FLT_1D_TYPE | s | Time |
transport_solver_numerics.time_step_min (alpha) | STRUCTURE | s | Minimum internal time step used by the transport solver between the previous and the current time stored for this quantity (assuming all transport equations are solved with the same time step) | |
transport_solver_numerics.time_step_min.data (alpha) | [transport_solver_numerics.time_step_min.time] | FLT_1D (uncertain) | s | Data |
transport_solver_numerics.time_step_min.time (alpha) | [1...N] | FLT_1D_TYPE | s | Time |
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 viewing 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) |