distribution_sources¶
Sources of particles for input to kinetic equations, e.g. Fokker-Planck calculation. The sources could originate from e.g. NBI or fusion reactions.
Maximum occurrences (MDS+ backend only): 4
New in version 3.2.1: lifecycle status alpha
Changed in version 4.1.0.
ids_propertiesstructure¶
See common IDS structure reference: ids_properties.
source(i1)AoS¶Set of source/sink terms. […]
Set of source/sink terms. A source/sink term corresponds to the particle source due to an NBI injection unit, a nuclear reaction or any combination of them (described in “identifier”)
Appendable by appender actor: yes
Maximum occurrences (MDS+ backend only): 33
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source(i1)/process(i2)AoS¶Set of processes (NBI units, fusion reactions, …) that provide […]
Set of processes (NBI units, fusion reactions, …) that provide the source.
Maximum occurrences (MDS+ backend only): 32
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source(i1)/process(i2)/typestructure¶Process type. […]
Process type. index=1 for NBI; index=2 for nuclear reaction (reaction unspecified); index=3 for nuclear reaction: T(d,n)4He [D+T->He4+n]; index=4 for nuclear reaction: He3(d,p)4He [He3+D->He4+p]; index=5 for nuclear reaction: D(d,p)T [D+D->T+p]; index=6 for nuclear reaction: D(d,n)3He [D+D->He3+n]; index=7 for runaway processes
This is an identifier. See distribution_source_identifier for the available options.
source(i1)/process(i2)/reactant_energystructure¶For nuclear reaction source, energy of the reactants. […]
For nuclear reaction source, energy of the reactants. index = 0 for a sum over all energies; index = 1 for thermal-thermal; index = 2 for beam-beam; index = 3 for beam-thermal
source(i1)/process(i2)/nbi_energystructure¶For NBI source, energy of the accelerated species considered. […]
For NBI source, energy of the accelerated species considered. index = 0 for a sum over all energies; index = 1 for full energiy; index = 2 for half energy; index = 3 for third energy
source(i1)/gyro_typeINT_0D¶Defines how to interpret the spatial coordinates: 1 = given at […]
Defines how to interpret the spatial coordinates: 1 = given at the actual particle birth point; 2 =given at the gyro centre of the birth point
source(i1)/speciesstructure¶Species injected or consumed by this source/sink
Species injected or consumed by this source/sink
source(i1)/species/typestructure¶Species type. […]
Species type. index=1 for electron; index=2 for ion species in a single/average state (refer to ion structure); index=3 for ion species in a particular state (refer to ion/state structure); index=4 for neutral species in a single/average state (refer to neutral structure); index=5 for neutral species in a particular state (refer to neutral/state structure); index=6 for neutron; index=7 for photon
This is an identifier. See species_reference_identifier for the available options.
source(i1)/species/ionstructure¶Description of the ion or neutral species, used if type/index […]
Description of the ion or neutral species, used if type/index = 2 or 3
source(i1)/species/ion/element(i2)AoS¶List of elements forming the atom or molecule
List of elements forming the atom or molecule
Maximum occurrences (MDS+ backend only): 5
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source(i1)/species/ion/z_ion ⇹eFLT_0D¶Ion charge (of the dominant ionization state; lumped ions are […]
Ion charge (of the dominant ionization state; lumped ions are allowed)
source(i1)/species/ion/nameSTR_0D¶String identifying ion (e.g. […]
String identifying ion (e.g. H+, D+, T+, He+2, C+, …)
Changed in version 3.42.0: Renamed from label
source(i1)/species/ion/statestructure¶Quantities related to the different states of the species (ionization, […]
Quantities related to the different states of the species (ionization, energy, excitation, …)
source(i1)/species/ion/state/z_min ⇹eFLT_0D¶Minimum Z of the charge state bundle (z_min = z_max = 0 for a […]
Minimum Z of the charge state bundle (z_min = z_max = 0 for a neutral)
source(i1)/species/ion/state/z_max ⇹eFLT_0D¶Maximum Z of the charge state bundle (equal to z_min if no bundle)
Maximum Z of the charge state bundle (equal to z_min if no bundle)
source(i1)/species/ion/state/nameSTR_0D¶String identifying ion state (e.g. […]
String identifying ion state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, …)
Changed in version 3.42.0: Renamed from label
source(i1)/species/ion/state/electron_configurationSTR_0D¶Configuration of atomic orbitals of this state, e.g. […]
Configuration of atomic orbitals of this state, e.g. 1s2-2s1
source(i1)/species/neutralstructure¶Description of the neutral species, used if type/index = 4 or […]
Description of the neutral species, used if type/index = 4 or 5
source(i1)/species/neutral/element(i2)AoS¶List of elements forming the atom or molecule
List of elements forming the atom or molecule
Maximum occurrences (MDS+ backend only): 5
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source(i1)/species/neutral/nameSTR_0D¶String identifying neutral (e.g. […]
String identifying neutral (e.g. H, D, T, He, C, …)
Changed in version 3.42.0: Renamed from label
source(i1)/species/neutral/statestructure¶State of the species (energy, excitation, …)
State of the species (energy, excitation, …)
source(i1)/species/neutral/state/nameSTR_0D¶String identifying neutral state
String identifying neutral state
Changed in version 3.42.0: Renamed from label
source(i1)/species/neutral/state/electron_configurationSTR_0D¶Configuration of atomic orbitals of this state, e.g. […]
Configuration of atomic orbitals of this state, e.g. 1s2-2s1
source(i1)/species/neutral/state/vibrational_level ⇹eFLT_0D¶Vibrational level (can be bundled)
Vibrational level (can be bundled)
source(i1)/species/neutral/state/vibrational_modeSTR_0D¶Vibrational mode of this state, e.g. […]
Vibrational mode of this state, e.g. “A_g”. Need to define, or adopt a standard nomenclature.
source(i1)/species/neutral/state/neutral_typestructure¶Neutral type, in terms of energy. […]
Neutral type, in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI
This is an identifier. See neutrals_identifier for the available options.
source(i1)/species/neutral/state/neutral_type/nameSTR_0D¶Short string identifier
Short string identifier
source(i1)/global_quantities(itime)AoS¶Global quantities for various time slices
Global quantities for various time slices
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source(i1)/global_quantities(itime)/power ⇹WFLT_0D¶Total power of the source
Total power of the source
source(i1)/global_quantities(itime)/torque_phi ⇹N.mFLT_0D¶Total toroidal torque of the source
Total toroidal torque of the source
Changed in version 3.42.0: Renamed from torque_tor
source(i1)/global_quantities(itime)/shinethroughstructure¶Shinethrough losses
Shinethrough losses
source(i1)/global_quantities(itime)/shinethrough/power ⇹WFLT_0D¶Power losses due to shinethrough
Power losses due to shinethrough
source(i1)/profiles_1d(itime)AoS¶Source radial profiles (flux surface averaged quantities) for […]
Source radial profiles (flux surface averaged quantities) for various time slices
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source(i1)/profiles_1d(itime)/gridstructure¶Radial grid
Radial grid
source(i1)/profiles_1d(itime)/grid/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate. […]
Normalized 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)
Alternatives for this coordinate
The following items may be used as a coordinate instead of rho_tor_norm:
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source(i1)/profiles_1d(itime)/grid/rho_tor(:) ⇹mFLT_1D¶Toroidal flux coordinate = sqrt(phi/(pi\*b0)), where the toroidal […]
Toroidal flux coordinate = sqrt(phi/(pi*b0)), where the toroidal magnetic field, b0, corresponds to that stored in vacuum_toroidal_field/b0 and pi can be found in the IMAS constants
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source(i1)/profiles_1d(itime)/grid/rho_pol_norm(:) ⇹1FLT_1D¶Normalized poloidal flux coordinate = sqrt((psi(rho)-psi(magnetic_axis)) […]
Normalized poloidal flux coordinate = sqrt((psi(rho)-psi(magnetic_axis)) / (psi(LCFS)-psi(magnetic_axis)))
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source(i1)/profiles_1d(itime)/grid/psi(:) ⇹WbFLT_1D¶Poloidal magnetic flux. […]
Poloidal magnetic flux. Integral of magnetic field passing through a contour defined by the intersection of a flux surface passing through the point of interest and a Z=constant plane. If the integration surface is flat, the surface normal vector is in the increasing vertical coordinate direction, Z, namely upwards.
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source(i1)/profiles_1d(itime)/grid/volume(:) ⇹m^3FLT_1D¶Volume enclosed inside the magnetic surface
Volume enclosed inside the magnetic surface
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source(i1)/profiles_1d(itime)/grid/area(:) ⇹m^2FLT_1D¶Cross-sectional area of the flux surface
Cross-sectional area of the flux surface
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source(i1)/profiles_1d(itime)/grid/surface(:) ⇹m^2FLT_1D¶Surface area of the toroidal flux surface
Surface area of the toroidal flux surface
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source(i1)/profiles_1d(itime)/grid/psi_magnetic_axis ⇹WbFLT_0D¶Value of the poloidal magnetic flux at the magnetic axis (useful […]
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)
source(i1)/profiles_1d(itime)/grid/psi_boundary ⇹WbFLT_0D¶Value of the poloidal magnetic flux at the plasma boundary (useful […]
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)
source(i1)/profiles_1d(itime)/energy(:) ⇹W.m^-3FLT_1D¶Source term for the energy transport equation
Source term for the energy transport equation
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source(i1)/profiles_1d(itime)/momentum_phi(:) ⇹N.m^-2FLT_1D¶Source term for the toroidal momentum equation
Source term for the toroidal momentum equation
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Changed in version 3.42.0: Renamed from momentum_tor
source(i1)/profiles_1d(itime)/particles(:) ⇹s^-1.m^-3FLT_1D¶Source term for the density transport equation
Source term for the density transport equation
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source(i1)/ggd(itime)AoS¶Source terms in phase space (real space, velocity space, spin […]
Source terms in phase space (real space, velocity space, spin state), represented using the ggd, for various time slices
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source(i1)/ggd(itime)/gridstructure¶Grid description
Grid description
source(i1)/ggd(itime)/grid/identifierstructure¶Grid identifier
Grid identifier
This is an identifier. See ggd_identifier for the available options.
source(i1)/ggd(itime)/grid/pathSTR_0D¶Path of the grid, including the IDS name, in case of implicit […]
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:2/description_ggd(1)/grid_ggd, means that the grid is located in the wall IDS, occurrence 2, with relative path description_ggd(1)/grid_ggd, using Fortran index convention (here : first index of the array)
source(i1)/ggd(itime)/grid/space(i2)AoS¶Set of grid spaces
Set of grid spaces
Click here for further documentation (or contact imas@iter.org if you can’t access this page).
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source(i1)/ggd(itime)/grid/space(i2)/identifierstructure¶Space identifier
Space identifier
This is an identifier. See ggd_space_identifier for the available options.
source(i1)/ggd(itime)/grid/space(i2)/identifier/nameSTR_0D¶Short string identifier
Short string identifier
source(i1)/ggd(itime)/grid/space(i2)/geometry_typestructure¶Type of space geometry (0: standard, 1:Fourier, >1: Fourier with […]
Type of space geometry (0: standard, 1:Fourier, >1: Fourier with periodicity)
source(i1)/ggd(itime)/grid/space(i2)/geometry_type/nameSTR_0D¶Short string identifier
Short string identifier
source(i1)/ggd(itime)/grid/space(i2)/coordinates_type(i3)AoS¶Type of coordinates describing the physical space, for every […]
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.
This is an identifier. See coordinate_identifier for the available options.
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Changed in version 4.0.0: Type changed from INT_1D
source(i1)/ggd(itime)/grid/space(i2)/coordinates_type(i3)/nameSTR_0D¶Short string identifier
Short string identifier
source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)AoS¶Definition of the space objects for every dimension (from one […]
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.
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source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/object(i4)AoS¶Set of objects for a given dimension
Set of objects for a given dimension
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source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/object(i4)/boundary(i5)AoS¶Set of (n-1)-dimensional objects defining the boundary of this […]
Set of (n-1)-dimensional objects defining the boundary of this n-dimensional object
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source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/object(i4)/boundary(i5)/indexINT_0D¶Index of this (n-1)-dimensional boundary object
Index of this (n-1)-dimensional boundary object
source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/object(i4)/boundary(i5)/neighbours(:)INT_1D¶List of indices of the n-dimensional objects adjacent to the […]
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
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source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/object(i4)/geometry(:)mixedFLT_1D¶Geometry data associated with the object, its detailed content […]
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.
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source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/object(i4)/nodes(:)INT_1D¶List of nodes forming this object (indices to objects_per_dimension(1)%object(:) […]
List of nodes forming this object (indices to objects_per_dimension(1)%object(:) in Fortran notation)
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source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/object(i4)/measurem^dimensionFLT_0D¶Measure of the space object, i.e. […]
Measure of the space object, i.e. physical size (length for 1d, area for 2d, volume for 3d objects,…)
source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/object(i4)/geometry_2d(:,:)mixedFLT_2D¶2D geometry data associated with the object. […]
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.
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New in version >3.35.0.
source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/geometry_contentstructure¶Content of the ../object/geometry node for this dimension
Content of the ../object/geometry node for this dimension
This is an identifier. See ggd_geometry_content_identifier for the available options.
New in version >3.33.0.
source(i1)/ggd(itime)/grid/space(i2)/objects_per_dimension(i3)/geometry_content/nameSTR_0D¶Short string identifier
Short string identifier
source(i1)/ggd(itime)/grid/grid_subset(i2)AoS¶Grid subsets
Grid subsets
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source(i1)/ggd(itime)/grid/grid_subset(i2)/identifierstructure¶Grid subset identifier
Grid subset identifier
Click here for further documentation.
This is an identifier. See ggd_subset_identifier for the available options.
source(i1)/ggd(itime)/grid/grid_subset(i2)/identifier/nameSTR_0D¶Short string identifier
Short string identifier
source(i1)/ggd(itime)/grid/grid_subset(i2)/dimensionINT_0D¶Space dimension of the grid subset elements, using the convention […]
Space dimension of the grid subset elements, using the convention 1=nodes, 2=edges, 3=faces, 4=cells/volumes
source(i1)/ggd(itime)/grid/grid_subset(i2)/element(i3)AoS¶Set of elements defining the grid subset. […]
Set of elements defining the grid subset. An element is defined by a combination of objects from potentially all spaces
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source(i1)/ggd(itime)/grid/grid_subset(i2)/element(i3)/object(i4)AoS¶Set of objects defining the element
Set of objects defining the element
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source(i1)/ggd(itime)/grid/grid_subset(i2)/element(i3)/object(i4)/spaceINT_0D¶Index of the space from which that object is taken
Index of the space from which that object is taken
source(i1)/ggd(itime)/grid/grid_subset(i2)/base(i3)AoS¶Set of bases for the grid subset. […]
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.
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source(i1)/ggd(itime)/grid/grid_subset(i2)/base(i3)/jacobian(:) ⇹mixedFLT_1D¶Metric Jacobian
Metric Jacobian
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source(i1)/ggd(itime)/grid/grid_subset(i2)/base(i3)/tensor_covariant(:,:,:) ⇹mixedFLT_3D¶Covariant metric tensor, given on each element of the subgrid […]
Covariant metric tensor, given on each element of the subgrid (first dimension)
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source(i1)/ggd(itime)/grid/grid_subset(i2)/base(i3)/tensor_contravariant(:,:,:) ⇹mixedFLT_3D¶Contravariant metric tensor, given on each element of the subgrid […]
Contravariant metric tensor, given on each element of the subgrid (first dimension)
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source(i1)/ggd(itime)/grid/grid_subset(i2)/metricstructure¶Metric of the canonical frame onto Cartesian coordinates
Metric of the canonical frame onto Cartesian coordinates
source(i1)/ggd(itime)/grid/grid_subset(i2)/metric/jacobian(:) ⇹mixedFLT_1D¶Metric Jacobian
Metric Jacobian
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source(i1)/ggd(itime)/grid/grid_subset(i2)/metric/tensor_covariant(:,:,:) ⇹mixedFLT_3D¶Covariant metric tensor, given on each element of the subgrid […]
Covariant metric tensor, given on each element of the subgrid (first dimension)
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source(i1)/ggd(itime)/grid/grid_subset(i2)/metric/tensor_contravariant(:,:,:) ⇹mixedFLT_3D¶Contravariant metric tensor, given on each element of the subgrid […]
Contravariant metric tensor, given on each element of the subgrid (first dimension)
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source(i1)/ggd(itime)/particles(i2)(m.s^-1)^-3.m^-3.s^-1AoS¶Source density of particles in phase space, for various grid […]
Source density of particles in phase space, for various grid subsets
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source(i1)/ggd(itime)/particles(i2)/grid_indexINT_0D¶Index of the grid used to represent this quantity
Index of the grid used to represent this quantity
source(i1)/ggd(itime)/particles(i2)/grid_subset_indexINT_0D¶Index of the grid subset the data is provided on. […]
Index of the grid subset the data is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index
source(i1)/ggd(itime)/particles(i2)/values(:) ⇹(m.s^-1)^-3.m^-3.s^-1FLT_1D¶One scalar value is provided per element in the grid subset.
One scalar value is provided per element in the grid subset.
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source(i1)/ggd(itime)/particles(i2)/coefficients(:,:) ⇹(m.s^-1)^-3.m^-3.s^-1FLT_2D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity with finite elements, provided per element in the grid subset (first dimension).
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source(i1)/ggd(itime)/discrete(:)INT_1D¶List of indices of grid spaces (refers to ../grid/space) for […]
List of indices of grid spaces (refers to ../grid/space) for which the source is discretely distributed. For example consider a source of 3.5 MeV alpha particles provided on a grid with two coordinates (spaces); rho_tor and energy. To specify that the source is given at energies exactly equal to 3.5 MeV, let discret have length 1 and set discrete(1)=2 since energy is dimension number 2. The source is then proportional to delta( 1 - energy / 3.5MeV ), where delta is the direct delta distribution. Discrete dimensions can only be used when the grid is rectangular.
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source(i1)/markers(itime)AoS¶Source given as a group of markers (test particles) born per […]
Source given as a group of markers (test particles) born per second, for various time slices
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source(i1)/markers(itime)/coordinate_identifier(i2)W.m^-3AoS¶Set of coordinate identifiers, coordinates on which the markers […]
Set of coordinate identifiers, coordinates on which the markers are represented
This is an identifier. See coordinate_identifier for the available options.
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source(i1)/markers(itime)/coordinate_identifier(i2)/nameSTR_0D¶Short string identifier
Short string identifier
source(i1)/markers(itime)/weights(:) ⇹1FLT_1D¶Weight of the markers, i.e. […]
Weight of the markers, i.e. number of real particles represented by each marker. The dimension of the vector correspond to the number of markers
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source(i1)/markers(itime)/positions(:,:) ⇹mixedFLT_2D¶Position of the markers in the set of coordinates. […]
Position of the markers in the set of coordinates. The first dimension corresponds to the number of markers, the second dimension to the set of coordinates
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source(i1)/markers(itime)/orbit_integralsstructure¶Integrals along the markers orbit. […]
Integrals along the markers orbit. These dimensionless expressions are of the form: (1/tau) integral (f(n_tor,m_pol,k,eq,…) dt) from time - tau to time, where tau is the transit/trapping time of the marker and f() a dimensionless function (phase factor,drift,etc) of the equilibrium (e.g. q) and perturbation (Fourier harmonics n_tor,m_pol and bounce harmonic k) along the particles orbits. In fact the integrals are taken during the last orbit of each marker at the time value of the time node below
source(i1)/markers(itime)/orbit_integrals/expressions(:)STR_1D¶List of the expressions f(n_tor,m_pol,k,q,…) used in the orbit […]
List of the expressions f(n_tor,m_pol,k,q,…) used in the orbit integrals
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source(i1)/markers(itime)/orbit_integrals/n_phi(:)INT_1D¶Array of toroidal mode numbers, where quantities vary as exp(i.n_phi.phi) […]
Array of toroidal mode numbers, where quantities vary as exp(i.n_phi.phi) and phi runs anticlockwise when viewed from above
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Changed in version 4.1.0: Renamed from n_tor
source(i1)/markers(itime)/orbit_integrals/m_pol(:)INT_1D¶Array of poloidal mode numbers, where quantities vary as exp(-i.m_pol.theta) […]
Array of poloidal mode numbers, where quantities vary as exp(-i.m_pol.theta) and theta is the angle defined by the choice of ../../coordinate_identifier, with its centre at the magnetic axis recalled at the root of this IDS
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source(i1)/markers(itime)/orbit_integrals/bounce_harmonics(:)INT_1D¶Array of bounce harmonics k
Array of bounce harmonics k
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source(i1)/markers(itime)/orbit_integrals_instantstructure¶Integrals/quantities along the markers orbit. […]
Integrals/quantities along the markers orbit. These dimensionless expressions are of the form: (1/tau) integral ( f(eq) dt) from time - tau to time_orbit for different values of time_orbit in the interval from time - tau to time, where tau is the transit/trapping time of the marker and f(eq) a dimensionless function (phase, drift,q,etc) of the equilibrium along the markers orbits. The integrals are taken during the last orbit of each marker at the time value of the time node below
source(i1)/markers(itime)/orbit_integrals_instant/expressions(:)STR_1D¶List of the expressions f(eq) used in the orbit integrals
List of the expressions f(eq) used in the orbit integrals
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source(i1)/markers(itime)/orbit_integrals_instant/time_orbit(:) ⇹sFLT_1D¶Time array along the markers last orbit
Time array along the markers last orbit
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source(i1)/markers(itime)/orbit_integrals_instant/values(:,:,:) ⇹1CPX_3D¶Values of the orbit integrals
Values of the orbit integrals
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source(i1)/markers(itime)/toroidal_modeINT_0D¶In case the orbit integrals are calculated for a given MHD perturbation, […]
In case the orbit integrals are calculated for a given MHD perturbation, index of the toroidal mode considered. Refers to the time_slice/toroidal_mode array of the MHD_LINEAR IDS in which this perturbation is described
vacuum_toroidal_fieldstructure¶Characteristics of the vacuum toroidal field (used in rho_tor […]
Characteristics of the vacuum toroidal field (used in rho_tor definition)
vacuum_toroidal_field/r0 ⇹mFLT_0D¶Reference major radius where the vacuum toroidal magnetic field […]
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)