core_profiles
¶
Core plasma profiles
Maximum occurrences (MDS+ backend only): 15
New in version 3.1.0: lifecycle status active
Changed in version 4.1.0.
ids_propertiesstructure¶
See common IDS structure reference: ids_properties
.
profiles_1d(itime)AoS¶Core plasma radial profiles for various time slices
Core plasma radial profiles for various time slices
1 |
profiles_1d(itime)/gridstructure¶Radial grid
Radial grid
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
:
1 |
|
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
1 |
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)))
1 |
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.
1 |
profiles_1d(itime)/grid/volume(:) ⇹m^3FLT_1D¶Volume enclosed inside the magnetic surface
Volume enclosed inside the magnetic surface
1 |
profiles_1d(itime)/grid/area(:) ⇹m^2FLT_1D¶Cross-sectional area of the flux surface
Cross-sectional area of the flux surface
1 |
profiles_1d(itime)/grid/surface(:) ⇹m^2FLT_1D¶Surface area of the toroidal flux surface
Surface area of the toroidal flux surface
1 |
profiles_1d(itime)/electronsstructure¶Quantities related to the electrons
Quantities related to the electrons
profiles_1d(itime)/electrons/temperature_validityINT_0D¶Indicator of the validity of the temperature profile. […]
Indicator of the validity of the temperature profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used
profiles_1d(itime)/electrons/temperature_fiteVstructure¶Information on the fit used to obtain the temperature profile
Information on the fit used to obtain the temperature profile
profiles_1d(itime)/electrons/temperature_fit/measured(:) ⇹mixedFLT_1D¶Measured values. […]
Measured values. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
|
profiles_1d(itime)/electrons/temperature_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […]
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
1 |
profiles_1d(itime)/electrons/temperature_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […]
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
1 |
profiles_1d(itime)/electrons/temperature_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […]
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/electrons/temperature_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/electrons/temperature_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […]
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
1 |
profiles_1d(itime)/electrons/temperature_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […]
Integer flag : 1 means local measurement, 0 means line-integrated measurement
1 |
profiles_1d(itime)/electrons/temperature_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […]
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
1 |
profiles_1d(itime)/electrons/temperature_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
1 |
profiles_1d(itime)/electrons/temperature_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit. […]
Value reconstructed from the fit. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
profiles_1d(itime)/electrons/temperature_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […]
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
1 |
profiles_1d(itime)/electrons/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal)
Density (thermal+non-thermal)
1 |
profiles_1d(itime)/electrons/density_validityINT_0D¶Indicator of the validity of the density profile. […]
Indicator of the validity of the density profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used
profiles_1d(itime)/electrons/density_fitm^-3structure¶Information on the fit used to obtain the density profile
Information on the fit used to obtain the density profile
profiles_1d(itime)/electrons/density_fit/measured(:) ⇹mixedFLT_1D¶Measured values. […]
Measured values. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
|
profiles_1d(itime)/electrons/density_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […]
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
1 |
profiles_1d(itime)/electrons/density_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […]
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
1 |
profiles_1d(itime)/electrons/density_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […]
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/electrons/density_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/electrons/density_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […]
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
1 |
profiles_1d(itime)/electrons/density_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […]
Integer flag : 1 means local measurement, 0 means line-integrated measurement
1 |
profiles_1d(itime)/electrons/density_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […]
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
1 |
profiles_1d(itime)/electrons/density_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
1 |
profiles_1d(itime)/electrons/density_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit. […]
Value reconstructed from the fit. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
profiles_1d(itime)/electrons/density_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […]
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
1 |
profiles_1d(itime)/electrons/density_thermal(:) ⇹m^-3FLT_1D¶Density of thermal particles
Density of thermal particles
1 |
profiles_1d(itime)/electrons/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles
Density of fast (non-thermal) particles
1 |
profiles_1d(itime)/electrons/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal)
Pressure (thermal+non-thermal)
1 |
profiles_1d(itime)/electrons/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2)
Pressure (thermal) associated with random motion ~average((v-average(v))^2)
1 |
profiles_1d(itime)/electrons/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure
Fast (non-thermal) perpendicular pressure
1 |
profiles_1d(itime)/electrons/pressure_fast_parallel(:) ⇹PaFLT_1D¶Fast (non-thermal) parallel pressure
Fast (non-thermal) parallel pressure
1 |
profiles_1d(itime)/ion(i1)AoS¶Quantities related to the different ion species, in the sense […]
Quantities related to the different ion species, in the sense of isonuclear or isomolecular sequences. Ionization states (or other types of states) must be differentiated at the state level below
1 |
|
profiles_1d(itime)/ion(i1)/element(i2)AoS¶List of elements forming the atom or molecule
List of elements forming the atom or molecule
1 |
|
profiles_1d(itime)/ion(i1)/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), volume averaged over plasma radius
profiles_1d(itime)/ion(i1)/nameSTR_0D¶String identifying ion (e.g. […]
String identifying ion (e.g. H, D, T, He, C, D2, …)
Changed in version 3.42.0: Renamed from label
profiles_1d(itime)/ion(i1)/neutral_indexINT_0D¶Index of the corresponding neutral species in the ../../neutral […]
Index of the corresponding neutral species in the ../../neutral array
profiles_1d(itime)/ion(i1)/z_ion_1d(:) ⇹1FLT_1D¶Average charge of the ion species (sum of states charge weighted […]
Average charge of the ion species (sum of states charge weighted by state density and divided by ion density)
1 |
profiles_1d(itime)/ion(i1)/z_ion_square_1d(:) ⇹1FLT_1D¶Average square charge of the ion species (sum of states square […]
Average square charge of the ion species (sum of states square charge weighted by state density and divided by ion density)
1 |
profiles_1d(itime)/ion(i1)/temperature(:) ⇹eVFLT_1D¶Temperature (average over charge states when multiple charge […]
Temperature (average over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/ion(i1)/temperature_validityINT_0D¶Indicator of the validity of the temperature profile. […]
Indicator of the validity of the temperature profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used
profiles_1d(itime)/ion(i1)/temperature_fiteVstructure¶Information on the fit used to obtain the temperature profile
Information on the fit used to obtain the temperature profile
profiles_1d(itime)/ion(i1)/temperature_fit/measured(:) ⇹mixedFLT_1D¶Measured values. […]
Measured values. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
|
profiles_1d(itime)/ion(i1)/temperature_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […]
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
1 |
profiles_1d(itime)/ion(i1)/temperature_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […]
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
1 |
profiles_1d(itime)/ion(i1)/temperature_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […]
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/ion(i1)/temperature_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/ion(i1)/temperature_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […]
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
1 |
profiles_1d(itime)/ion(i1)/temperature_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […]
Integer flag : 1 means local measurement, 0 means line-integrated measurement
1 |
profiles_1d(itime)/ion(i1)/temperature_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […]
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
1 |
profiles_1d(itime)/ion(i1)/temperature_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
1 |
profiles_1d(itime)/ion(i1)/temperature_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit. […]
Value reconstructed from the fit. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
profiles_1d(itime)/ion(i1)/temperature_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […]
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
1 |
profiles_1d(itime)/ion(i1)/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal) (sum over charge states when multiple […]
Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/ion(i1)/density_validityINT_0D¶Indicator of the validity of the density profile. […]
Indicator of the validity of the density profile. 0: valid from automated processing, 1: valid and certified by the RO; - 1 means problem identified in the data processing (request verification by the RO), -2: invalid data, should not be used
profiles_1d(itime)/ion(i1)/density_fitm^-3structure¶Information on the fit used to obtain the density profile
Information on the fit used to obtain the density profile
profiles_1d(itime)/ion(i1)/density_fit/measured(:) ⇹mixedFLT_1D¶Measured values. […]
Measured values. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
|
profiles_1d(itime)/ion(i1)/density_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […]
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
1 |
profiles_1d(itime)/ion(i1)/density_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […]
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
1 |
profiles_1d(itime)/ion(i1)/density_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […]
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/ion(i1)/density_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/ion(i1)/density_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […]
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
1 |
profiles_1d(itime)/ion(i1)/density_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […]
Integer flag : 1 means local measurement, 0 means line-integrated measurement
1 |
profiles_1d(itime)/ion(i1)/density_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […]
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
1 |
profiles_1d(itime)/ion(i1)/density_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
1 |
profiles_1d(itime)/ion(i1)/density_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit. […]
Value reconstructed from the fit. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
profiles_1d(itime)/ion(i1)/density_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […]
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
1 |
profiles_1d(itime)/ion(i1)/density_thermal(:) ⇹m^-3FLT_1D¶Density (thermal) (sum over charge states when multiple charge […]
Density (thermal) (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/ion(i1)/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles (sum over charge states […]
Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/ion(i1)/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal) (sum over charge states when multiple […]
Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/ion(i1)/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2) […]
Pressure (thermal) associated with random motion ~average((v-average(v))^2) (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/ion(i1)/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure (sum over charge states […]
Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/ion(i1)/pressure_fast_parallel(:) ⇹PaFLT_1D¶Fast (non-thermal) parallel pressure (sum over charge states […]
Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/ion(i1)/rotation_frequency_tor(:) ⇹rad.s^-1FLT_1D¶Toroidal rotation frequency (i.e. […]
Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken) (average over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/ion(i1)/velocitym.s^-1structure¶Velocity (average over charge states when multiple charge states […]
Velocity (average over charge states when multiple charge states are considered) at the position of maximum major radius on every flux surface
profiles_1d(itime)/ion(i1)/velocity/diamagnetic(:) ⇹m.s^-1FLT_1D¶Diamagnetic component
Diamagnetic component
1 |
profiles_1d(itime)/ion(i1)/velocity/parallel(:) ⇹m.s^-1FLT_1D¶Parallel component
Parallel component
1 |
profiles_1d(itime)/ion(i1)/velocity/poloidal(:) ⇹m.s^-1FLT_1D¶Poloidal component
Poloidal component
1 |
profiles_1d(itime)/ion(i1)/multiple_states_flagINT_0D¶Multiple states calculation flag : 0-Only the ‘ion’ level is […]
Multiple states calculation flag : 0-Only the ‘ion’ level is considered and the ‘state’ array of structure is empty; 1-Ion states are considered and are described in the ‘state’ array of structure
profiles_1d(itime)/ion(i1)/state(i2)AoS¶Quantities related to the different states of the species (ionization, […]
Quantities related to the different states of the species (ionization, energy, excitation, …)
1 |
|
profiles_1d(itime)/ion(i1)/state(i2)/z_min ⇹eFLT_0D¶Minimum Z of the charge state bundle
Minimum Z of the charge state bundle
profiles_1d(itime)/ion(i1)/state(i2)/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)
profiles_1d(itime)/ion(i1)/state(i2)/z_average ⇹eFLT_0D¶Average Z of the charge state bundle, volume averaged over the […]
Average Z of the charge state bundle, volume averaged over the plasma radius (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
profiles_1d(itime)/ion(i1)/state(i2)/z_square_average ⇹eFLT_0D¶Average Z square of the charge state bundle, volume averaged […]
Average Z square of the charge state bundle, volume averaged over the plasma radius (equal to z_min squared if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
profiles_1d(itime)/ion(i1)/state(i2)/z_average_1d(:) ⇹1FLT_1D¶Average charge profile of the charge state bundle (equal to z_min […]
Average charge profile of the charge state bundle (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
1 |
profiles_1d(itime)/ion(i1)/state(i2)/z_average_square_1d(:) ⇹1FLT_1D¶Average square charge profile of the charge state bundle (equal […]
Average square charge profile of the charge state bundle (equal to z_min squared if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
1 |
profiles_1d(itime)/ion(i1)/state(i2)/ionization_potential ⇹eVFLT_0D¶Cumulative and average ionization potential to reach a given […]
Cumulative and average ionization potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z’=0 to z-1)), where Epot is the ionization potential of ion Xz’+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
Changed in version 4.0.0: Renamed from ionisation_potential
profiles_1d(itime)/ion(i1)/state(i2)/nameSTR_0D¶String identifying state (e.g. […]
String identifying state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, …)
Changed in version 3.42.0: Renamed from label
profiles_1d(itime)/ion(i1)/state(i2)/electron_configurationSTR_0D¶Configuration of atomic orbitals of this state, e.g. […]
Configuration of atomic orbitals of this state, e.g. 1s2-2s1
profiles_1d(itime)/ion(i1)/state(i2)/vibrational_level ⇹eFLT_0D¶Vibrational level (can be bundled)
Vibrational level (can be bundled)
profiles_1d(itime)/ion(i1)/state(i2)/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.
profiles_1d(itime)/ion(i1)/state(i2)/rotation_frequency_tor(:) ⇹rad.s^-1FLT_1D¶Toroidal rotation frequency (i.e. […]
Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken)
1 |
profiles_1d(itime)/ion(i1)/state(i2)/velocitym.s^-1structure¶Velocity at the position of maximum major radius on every flux […]
Velocity at the position of maximum major radius on every flux surface
New in version >4.0.0.
profiles_1d(itime)/ion(i1)/state(i2)/velocity/radial(:) ⇹m.s^-1FLT_1D¶Radial component
Radial component
1 |
profiles_1d(itime)/ion(i1)/state(i2)/velocity/diamagnetic(:) ⇹m.s^-1FLT_1D¶Diamagnetic component
Diamagnetic component
1 |
profiles_1d(itime)/ion(i1)/state(i2)/velocity/parallel(:) ⇹m.s^-1FLT_1D¶Parallel component
Parallel component
1 |
profiles_1d(itime)/ion(i1)/state(i2)/velocity/poloidal(:) ⇹m.s^-1FLT_1D¶Poloidal component
Poloidal component
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal)
Density (thermal+non-thermal)
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_fitm^-3structure¶Information on the fit used to obtain the density profile
Information on the fit used to obtain the density profile
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/measured(:) ⇹mixedFLT_1D¶Measured values. […]
Measured values. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
|
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […]
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […]
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […]
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […]
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […]
Integer flag : 1 means local measurement, 0 means line-integrated measurement
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […]
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit. […]
Value reconstructed from the fit. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […]
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_thermal(:) ⇹m^-3FLT_1D¶Density of thermal particles
Density of thermal particles
1 |
profiles_1d(itime)/ion(i1)/state(i2)/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles
Density of fast (non-thermal) particles
1 |
profiles_1d(itime)/ion(i1)/state(i2)/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal)
Pressure (thermal+non-thermal)
1 |
profiles_1d(itime)/ion(i1)/state(i2)/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2)
Pressure (thermal) associated with random motion ~average((v-average(v))^2)
1 |
profiles_1d(itime)/ion(i1)/state(i2)/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure
Fast (non-thermal) perpendicular pressure
1 |
profiles_1d(itime)/neutral(i1)AoS¶Quantities related to the different neutral species
Quantities related to the different neutral species
1 |
|
profiles_1d(itime)/neutral(i1)/element(i2)AoS¶List of elements forming the atom or molecule
List of elements forming the atom or molecule
1 |
|
profiles_1d(itime)/neutral(i1)/nameSTR_0D¶String identifying the species (e.g. […]
String identifying the species (e.g. H, D, T, He, C, D2, DT, CD4, …)
Changed in version 3.42.0: Renamed from label
profiles_1d(itime)/neutral(i1)/ion_indexINT_0D¶Index of the corresponding ion species in the ../../ion array
Index of the corresponding ion species in the ../../ion array
profiles_1d(itime)/neutral(i1)/temperature(:) ⇹eVFLT_1D¶Temperature (average over charge states when multiple charge […]
Temperature (average over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/neutral(i1)/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal) (sum over charge states when multiple […]
Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/neutral(i1)/density_thermal(:) ⇹m^-3FLT_1D¶Density (thermal) (sum over charge states when multiple charge […]
Density (thermal) (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/neutral(i1)/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles (sum over charge states […]
Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/neutral(i1)/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal) (sum over charge states when multiple […]
Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/neutral(i1)/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2) […]
Pressure (thermal) associated with random motion ~average((v-average(v))^2) (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/neutral(i1)/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure (sum over charge states […]
Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/neutral(i1)/pressure_fast_parallel(:) ⇹PaFLT_1D¶Fast (non-thermal) parallel pressure (sum over charge states […]
Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered)
1 |
profiles_1d(itime)/neutral(i1)/multiple_states_flagINT_0D¶Multiple states calculation flag : 0-Only one state is considered; […]
Multiple states calculation flag : 0-Only one state is considered; 1-Multiple states are considered and are described in the state structure
profiles_1d(itime)/neutral(i1)/state(i2)AoS¶Quantities related to the different states of the species (energy, […]
Quantities related to the different states of the species (energy, excitation, …)
1 |
|
profiles_1d(itime)/neutral(i1)/state(i2)/nameSTR_0D¶String identifying state
String identifying state
Changed in version 3.42.0: Renamed from label
profiles_1d(itime)/neutral(i1)/state(i2)/electron_configurationSTR_0D¶Configuration of atomic orbitals of this state, e.g. […]
Configuration of atomic orbitals of this state, e.g. 1s2-2s1
profiles_1d(itime)/neutral(i1)/state(i2)/vibrational_level ⇹eFLT_0D¶Vibrational level (can be bundled)
Vibrational level (can be bundled)
profiles_1d(itime)/neutral(i1)/state(i2)/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.
profiles_1d(itime)/neutral(i1)/state(i2)/neutral_typestructure¶Neutral type (if the considered state is a neutral), in terms […]
Neutral type (if the considered state is a neutral), in terms of energy. ID =1: cold; 2: thermal; 3: fast; 4: NBI
This is an identifier. See neutrals_identifier
for the available options.
profiles_1d(itime)/neutral(i1)/state(i2)/neutral_type/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/neutral(i1)/state(i2)/density(:) ⇹m^-3FLT_1D¶Density (thermal+non-thermal)
Density (thermal+non-thermal)
1 |
profiles_1d(itime)/neutral(i1)/state(i2)/density_thermal(:) ⇹m^-3FLT_1D¶Density of thermal particles
Density of thermal particles
1 |
profiles_1d(itime)/neutral(i1)/state(i2)/density_fast(:) ⇹m^-3FLT_1D¶Density of fast (non-thermal) particles
Density of fast (non-thermal) particles
1 |
profiles_1d(itime)/neutral(i1)/state(i2)/pressure(:) ⇹PaFLT_1D¶Pressure (thermal+non-thermal)
Pressure (thermal+non-thermal)
1 |
profiles_1d(itime)/neutral(i1)/state(i2)/pressure_thermal(:) ⇹PaFLT_1D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2)
Pressure (thermal) associated with random motion ~average((v-average(v))^2)
1 |
profiles_1d(itime)/neutral(i1)/state(i2)/pressure_fast_perpendicular(:) ⇹PaFLT_1D¶Fast (non-thermal) perpendicular pressure
Fast (non-thermal) perpendicular pressure
1 |
profiles_1d(itime)/t_i_average(:) ⇹eVFLT_1D¶Ion temperature (averaged on charge states and ion species)
Ion temperature (averaged on charge states and ion species)
1 |
profiles_1d(itime)/t_i_average_fiteVstructure¶Information on the fit used to obtain the t_i_average profile
Information on the fit used to obtain the t_i_average profile
profiles_1d(itime)/t_i_average_fit/measured(:) ⇹mixedFLT_1D¶Measured values. […]
Measured values. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
|
profiles_1d(itime)/t_i_average_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […]
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
1 |
profiles_1d(itime)/t_i_average_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […]
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
1 |
profiles_1d(itime)/t_i_average_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […]
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/t_i_average_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/t_i_average_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […]
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
1 |
profiles_1d(itime)/t_i_average_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […]
Integer flag : 1 means local measurement, 0 means line-integrated measurement
1 |
profiles_1d(itime)/t_i_average_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […]
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
1 |
profiles_1d(itime)/t_i_average_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
1 |
profiles_1d(itime)/t_i_average_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit. […]
Value reconstructed from the fit. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
profiles_1d(itime)/t_i_average_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […]
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
1 |
profiles_1d(itime)/n_i_total_over_n_e(:) ⇹1FLT_1D¶Ratio of total ion density (sum over species and charge states) […]
Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal)
1 |
profiles_1d(itime)/n_i_thermal_total(:) ⇹m^-3FLT_1D¶Total ion thermal density (sum over species and charge states)
Total ion thermal density (sum over species and charge states)
1 |
profiles_1d(itime)/momentum_phi(:) ⇹kg.m^-1.s^-1FLT_1D¶Total plasma toroidal momentum, summed over ion species and electrons […]
Total plasma toroidal momentum, summed over ion species and electrons weighted by their density and major radius, i.e. sum_over_species(n*R*m*Vphi)
1 |
Changed in version 3.42.0: Renamed from momentum_tor
profiles_1d(itime)/zeff_fit1structure¶Information on the fit used to obtain the zeff profile
Information on the fit used to obtain the zeff profile
profiles_1d(itime)/zeff_fit/measured(:) ⇹mixedFLT_1D¶Measured values. […]
Measured values. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
|
profiles_1d(itime)/zeff_fit/source(:)STR_1D¶Path to the source data for each measurement in the IMAS data […]
Path to the source data for each measurement in the IMAS data dictionary, e.g. ece/channel(i)/t_e for the electron temperature on the i-th channel in the ECE IDS
1 |
profiles_1d(itime)/zeff_fit/time_measurement(:) ⇹sFLT_1D¶Exact time slices used from the time array of the measurement […]
Exact time slices used from the time array of the measurement source data. The time slice is indicated for each measurement point considered in the fit since measurements may come from different and thus asynchronous diagnostics. If the time slice does not exist in the time array of the source data, it means linear interpolation has been used
1 |
profiles_1d(itime)/zeff_fit/time_measurement_slice_methodstructure¶Method used to slice the data : index = 0 means using exact time […]
Method used to slice the data : index = 0 means using exact time slice of the measurement, 1 means linear interpolation, …
profiles_1d(itime)/zeff_fit/time_measurement_slice_method/nameSTR_0D¶Short string identifier
Short string identifier
profiles_1d(itime)/zeff_fit/time_measurement_width(:) ⇹sFLT_1D¶In case the measurements are averaged over a time interval, this […]
In case the measurements are averaged over a time interval, this node is the full width of this time interval (empty otherwise). In case the slicing/averaging method doesn’t use a hard time interval cutoff, this width is the characteristic time span of the slicing/averaging method. By convention, the time interval starts at time_measurement-time_width and ends at time_measurement.
1 |
profiles_1d(itime)/zeff_fit/local(:)INT_1D¶Integer flag : 1 means local measurement, 0 means line-integrated […]
Integer flag : 1 means local measurement, 0 means line-integrated measurement
1 |
profiles_1d(itime)/zeff_fit/rho_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal flux coordinate of each measurement (local […]
Normalized toroidal flux coordinate of each measurement (local value for a local measurement, minimum value reached by the line of sight for a line measurement)
1 |
profiles_1d(itime)/zeff_fit/weight(:) ⇹1FLT_1D¶Weight given to each measured value
Weight given to each measured value
1 |
profiles_1d(itime)/zeff_fit/reconstructed(:) ⇹mixedFLT_1D¶Value reconstructed from the fit. […]
Value reconstructed from the fit. Units are: as_parent for a local measurement, as_parent.m for a line integrated measurement.
1 |
profiles_1d(itime)/zeff_fit/chi_squared(:) ⇹1FLT_1D¶Squared error normalized by the weighted standard deviation considered […]
Squared error normalized by the weighted standard deviation considered in the minimization process : chi_squared = weight^2 *(reconstructed - measured)^2 / sigma^2, where sigma is the standard deviation of the measurement error
1 |
profiles_1d(itime)/pressure_ion_total(:) ⇹PaFLT_1D¶Total (sum over ion species) thermal ion pressure
Total (sum over ion species) thermal ion pressure
1 |
profiles_1d(itime)/pressure_thermal(:) ⇹PaFLT_1D¶Thermal pressure (electrons+ions)
Thermal pressure (electrons+ions)
1 |
profiles_1d(itime)/pressure_perpendicular(:) ⇹PaFLT_1D¶Total perpendicular pressure (electrons+ions, thermal+non-thermal)
Total perpendicular pressure (electrons+ions, thermal+non-thermal)
1 |
profiles_1d(itime)/pressure_parallel(:) ⇹PaFLT_1D¶Total parallel pressure (electrons+ions, thermal+non-thermal)
Total parallel pressure (electrons+ions, thermal+non-thermal)
1 |
profiles_1d(itime)/j_total(:) ⇹A.m^-2FLT_1D¶Total parallel current density = average(jtot.B) / B0, where […]
Total parallel current density = average(jtot.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0
1 |
profiles_1d(itime)/current_parallel_inside(:) ⇹AFLT_1D¶Parallel current driven inside the flux surface. […]
Parallel current driven inside the flux surface. Cumulative surface integral of j_total
1 |
profiles_1d(itime)/j_phi(:) ⇹A.m^-2FLT_1D¶Total toroidal current density = average(J_phi/R) / average(1/R)
Total toroidal current density = average(J_phi/R) / average(1/R)
1 |
Changed in version 3.42.0: Renamed from j_tor
profiles_1d(itime)/j_ohmic(:) ⇹A.m^-2FLT_1D¶Ohmic parallel current density = average(J_Ohmic.B) / B0, where […]
Ohmic parallel current density = average(J_Ohmic.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0
1 |
profiles_1d(itime)/j_non_inductive(:) ⇹A.m^-2FLT_1D¶Non-inductive (includes bootstrap) parallel current density = […]
Non-inductive (includes bootstrap) parallel current density = average(jni.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0
1 |
profiles_1d(itime)/j_bootstrap(:) ⇹A.m^-2FLT_1D¶Bootstrap current density = average(J_Bootstrap.B) / B0, where […]
Bootstrap current density = average(J_Bootstrap.B) / B0, where B0 = Core_Profiles/Vacuum_Toroidal_Field/ B0
1 |
profiles_1d(itime)/conductivity_parallel(:) ⇹ohm^-1.m^-1FLT_1D¶Parallel conductivity
Parallel conductivity
1 |
profiles_1d(itime)/e_fieldV.m^-1structure¶Electric field, averaged on the magnetic surface. […]
Electric field, averaged on the magnetic surface. E.g for the parallel component, average(E.B) / B0, using core_profiles/vacuum_toroidal_field/b0
profiles_1d(itime)/e_field/diamagnetic(:) ⇹V.m^-1FLT_1D¶Diamagnetic component
Diamagnetic component
1 |
profiles_1d(itime)/phi_potential(:) ⇹VFLT_1D¶Electrostatic potential, averaged on the magnetic flux surface
Electrostatic potential, averaged on the magnetic flux surface
1 |
profiles_1d(itime)/rotation_frequency_tor_sonic(:) ⇹s^-1FLT_1D¶Derivative of the flux surface averaged electrostatic potential […]
Derivative of the flux surface averaged electrostatic potential with respect to the poloidal flux, multiplied by (1/2pi). This quantity is the toroidal angular rotation frequency due to the ExB drift, introduced in formula (43) of Hinton and Wong, Physics of Fluids 3082 (1985), also referred to as sonic flow in regimes in which the toroidal velocity is dominant over the poloidal velocity
Click here for further documentation.
1 |
profiles_1d(itime)/q(:) ⇹1FLT_1D¶Safety factor (only positive when toroidal current and magnetic […]
Safety factor (only positive when toroidal current and magnetic field are in same direction)
1 |
profiles_2d(itime)AoS¶Core plasma quantities in a poloidal cross section, for various […]
Core plasma quantities in a poloidal cross section, for various time slices
1 |
New in version 3.39.0: lifecycle status alpha
New in version >3.38.1.
profiles_2d(itime)/grid_typestructure¶Selection of one of a set of grid types
Selection of one of a set of grid types
This is an identifier. See poloidal_plane_coordinates_identifier
for the available options.
profiles_2d(itime)/gridstructure¶Definition of the 2D grid (the content of dim1 and dim2 is defined […]
Definition of the 2D grid (the content of dim1 and dim2 is defined by the selected grid_type)
profiles_2d(itime)/grid/dim2(:) ⇹mixedFLT_1D¶Second dimension values
Second dimension values
1 |
|
profiles_2d(itime)/ion(i1)AoS¶2D quantities related to the different ion species, in the sense […]
2D quantities related to the different ion species, in the sense of isonuclear or isomolecular sequences. Ionization states (or other types of states) must be differentiated at the state level below. This array doesn’t necessarily have the same size as the profiles_1d/ion array, since 2D data may be relevant only for a subset of ion species.
1 |
|
profiles_2d(itime)/ion(i1)/element(i2)AoS¶List of elements forming the atom or molecule
List of elements forming the atom or molecule
1 |
|
profiles_2d(itime)/ion(i1)/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), volume averaged over plasma radius
profiles_2d(itime)/ion(i1)/nameSTR_0D¶String identifying ion (e.g. […]
String identifying ion (e.g. H, D, T, He, C, D2, …)
Changed in version 3.42.0: Renamed from label
profiles_2d(itime)/ion(i1)/ion_indexINT_0D¶Index of the corresponding ion species in the ../../../profiles_1d/ion […]
Index of the corresponding ion species in the ../../../profiles_1d/ion array
profiles_2d(itime)/ion(i1)/temperature(:,:) ⇹eVFLT_2D¶Temperature (average over charge states when multiple charge […]
Temperature (average over charge states when multiple charge states are considered)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/density(:,:) ⇹m^-3FLT_2D¶Density (thermal+non-thermal) (sum over charge states when multiple […]
Density (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/density_thermal(:,:) ⇹m^-3FLT_2D¶Density (thermal) (sum over charge states when multiple charge […]
Density (thermal) (sum over charge states when multiple charge states are considered)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/density_fast(:,:) ⇹m^-3FLT_2D¶Density of fast (non-thermal) particles (sum over charge states […]
Density of fast (non-thermal) particles (sum over charge states when multiple charge states are considered)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/pressure(:,:) ⇹PaFLT_2D¶Pressure (thermal+non-thermal) (sum over charge states when multiple […]
Pressure (thermal+non-thermal) (sum over charge states when multiple charge states are considered)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/pressure_thermal(:,:) ⇹PaFLT_2D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2) […]
Pressure (thermal) associated with random motion ~average((v-average(v))^2) (sum over charge states when multiple charge states are considered)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/pressure_fast_perpendicular(:,:) ⇹PaFLT_2D¶Fast (non-thermal) perpendicular pressure (sum over charge states […]
Fast (non-thermal) perpendicular pressure (sum over charge states when multiple charge states are considered)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/pressure_fast_parallel(:,:) ⇹PaFLT_2D¶Fast (non-thermal) parallel pressure (sum over charge states […]
Fast (non-thermal) parallel pressure (sum over charge states when multiple charge states are considered)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/rotation_frequency_tor(:,:) ⇹rad.s^-1FLT_2D¶Toroidal rotation frequency (i.e. […]
Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken) (average over charge states when multiple charge states are considered)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/velocitym.s^-1structure¶Velocity (average over charge states when multiple charge states […]
Velocity (average over charge states when multiple charge states are considered) at the position of maximum major radius on every flux surface
profiles_2d(itime)/ion(i1)/velocity/diamagnetic(:,:) ⇹m.s^-1FLT_2D¶Diamagnetic component
Diamagnetic component
1 |
|
2 |
profiles_2d(itime)/ion(i1)/velocity/parallel(:,:) ⇹m.s^-1FLT_2D¶Parallel component
Parallel component
1 |
|
2 |
profiles_2d(itime)/ion(i1)/velocity/poloidal(:,:) ⇹m.s^-1FLT_2D¶Poloidal component
Poloidal component
1 |
|
2 |
profiles_2d(itime)/ion(i1)/multiple_states_flagINT_0D¶Multiple states calculation flag : 0-Only the ‘ion’ level is […]
Multiple states calculation flag : 0-Only the ‘ion’ level is considered and the ‘state’ array of structure is empty; 1-Ion states are considered and are described in the ‘state’ array of structure
profiles_2d(itime)/ion(i1)/state(i2)AoS¶Quantities related to the different states of the species (ionization, […]
Quantities related to the different states of the species (ionization, energy, excitation, …)
1 |
|
profiles_2d(itime)/ion(i1)/state(i2)/z_min ⇹eFLT_0D¶Minimum Z of the charge state bundle
Minimum Z of the charge state bundle
profiles_2d(itime)/ion(i1)/state(i2)/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)
profiles_2d(itime)/ion(i1)/state(i2)/z_average ⇹eFLT_0D¶Average Z of the charge state bundle, volume averaged over the […]
Average Z of the charge state bundle, volume averaged over the plasma radius (equal to z_min if no bundle), = sum (Z*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
profiles_2d(itime)/ion(i1)/state(i2)/z_square_average ⇹eFLT_0D¶Average Z square of the charge state bundle, volume averaged […]
Average Z square of the charge state bundle, volume averaged over the plasma radius (equal to z_min squared if no bundle), = sum (Z^2*x_z) where x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
profiles_2d(itime)/ion(i1)/state(i2)/ionization_potential ⇹eVFLT_0D¶Cumulative and average ionization potential to reach a given […]
Cumulative and average ionization potential to reach a given bundle. Defined as sum (x_z* (sum of Epot from z’=0 to z-1)), where Epot is the ionization potential of ion Xz’+, and x_z is the relative concentration of a given charge state in the bundle, i.e. sum(x_z) = 1 over the bundle.
Changed in version 4.0.0: Renamed from ionisation_potential
profiles_2d(itime)/ion(i1)/state(i2)/nameSTR_0D¶String identifying state (e.g. […]
String identifying state (e.g. C+, C+2 , C+3, C+4, C+5, C+6, …)
Changed in version 3.42.0: Renamed from label
profiles_2d(itime)/ion(i1)/state(i2)/electron_configurationSTR_0D¶Configuration of atomic orbitals of this state, e.g. […]
Configuration of atomic orbitals of this state, e.g. 1s2-2s1
profiles_2d(itime)/ion(i1)/state(i2)/vibrational_level ⇹eFLT_0D¶Vibrational level (can be bundled)
Vibrational level (can be bundled)
profiles_2d(itime)/ion(i1)/state(i2)/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.
profiles_2d(itime)/ion(i1)/state(i2)/rotation_frequency_tor(:,:) ⇹rad.s^-1FLT_2D¶Toroidal rotation frequency (i.e. […]
Toroidal rotation frequency (i.e. toroidal velocity divided by the major radius at which the toroidal velocity is taken)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/state(i2)/density(:,:) ⇹m^-3FLT_2D¶Density (thermal+non-thermal)
Density (thermal+non-thermal)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/state(i2)/density_thermal(:,:) ⇹m^-3FLT_2D¶Density of thermal particles
Density of thermal particles
1 |
|
2 |
profiles_2d(itime)/ion(i1)/state(i2)/density_fast(:,:) ⇹m^-3FLT_2D¶Density of fast (non-thermal) particles
Density of fast (non-thermal) particles
1 |
|
2 |
profiles_2d(itime)/ion(i1)/state(i2)/pressure(:,:) ⇹PaFLT_2D¶Pressure (thermal+non-thermal)
Pressure (thermal+non-thermal)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/state(i2)/pressure_thermal(:,:) ⇹PaFLT_2D¶Pressure (thermal) associated with random motion ~average((v-average(v))^2)
Pressure (thermal) associated with random motion ~average((v-average(v))^2)
1 |
|
2 |
profiles_2d(itime)/ion(i1)/state(i2)/pressure_fast_perpendicular(:,:) ⇹PaFLT_2D¶Fast (non-thermal) perpendicular pressure
Fast (non-thermal) perpendicular pressure
1 |
|
2 |
profiles_2d(itime)/t_i_average(:,:) ⇹eVFLT_2D¶Ion temperature (averaged on states and ion species)
Ion temperature (averaged on states and ion species)
1 |
|
2 |
profiles_2d(itime)/n_i_total_over_n_e(:,:) ⇹1FLT_2D¶Ratio of total ion density (sum over species and charge states) […]
Ratio of total ion density (sum over species and charge states) over electron density. (thermal+non-thermal)
1 |
|
2 |
profiles_2d(itime)/n_i_thermal_total(:,:) ⇹m^-3FLT_2D¶Total ion thermal density (sum over species and charge states)
Total ion thermal density (sum over species and charge states)
1 |
|
2 |
profiles_2d(itime)/momentum_phi(:,:) ⇹kg.m^-1.s^-1FLT_2D¶Total plasma toroidal momentum, summed over ion species and electrons […]
Total plasma toroidal momentum, summed over ion species and electrons weighted by their density and major radius, i.e. sum_over_species(n*R*m*Vphi)
1 |
|
2 |
Changed in version 3.42.0: Renamed from momentum_tor
profiles_2d(itime)/pressure_ion_total(:,:) ⇹PaFLT_2D¶Total (sum over ion species) thermal ion pressure
Total (sum over ion species) thermal ion pressure
1 |
|
2 |
profiles_2d(itime)/pressure_thermal(:,:) ⇹PaFLT_2D¶Thermal pressure (electrons+ions)
Thermal pressure (electrons+ions)
1 |
|
2 |
profiles_2d(itime)/pressure_perpendicular(:,:) ⇹PaFLT_2D¶Total perpendicular pressure (electrons+ions, thermal+non-thermal)
Total perpendicular pressure (electrons+ions, thermal+non-thermal)
1 |
|
2 |
global_quantitiesstructure¶Various global quantities derived from the profiles
Various global quantities derived from the profiles
global_quantities/ip(:) ⇹AFLT_1D¶Total plasma current (toroidal component). […]
Total plasma current (toroidal component). Positive sign means anti-clockwise when viewed from above.
1 |
global_quantities/current_non_inductive(:) ⇹AFLT_1D¶Total non-inductive current (toroidal component). […]
Total non-inductive current (toroidal component). Positive sign means anti-clockwise when viewed from above.
1 |
global_quantities/current_bootstrap(:) ⇹AFLT_1D¶Bootstrap current (toroidal component). […]
Bootstrap current (toroidal component). Positive sign means anti-clockwise when viewed from above.
1 |
global_quantities/v_loop(:) ⇹VFLT_1D¶LCFS loop voltage (positive value drives positive ohmic current […]
LCFS loop voltage (positive value drives positive ohmic current that flows anti-clockwise when viewed from above)
1 |
global_quantities/li_3(:) ⇹1FLT_1D¶Internal inductance. […]
Internal inductance. The li_3 definition is used, i.e. li_3 = 2/R0/mu0^2/Ip^2 * int(Bp^2 dV).
1 |
global_quantities/beta_tor(:) ⇹1FLT_1D¶Toroidal beta, defined as the volume-averaged total perpendicular […]
Toroidal beta, defined as the volume-averaged total perpendicular pressure divided by (B0^2/(2*mu0)), i.e. beta_toroidal = 2 mu0 int(p dV) / V / B0^2
1 |
global_quantities/beta_tor_norm(:) ⇹1FLT_1D¶Normalized toroidal beta, defined as 100 \* beta_tor \* a[m] […]
Normalized toroidal beta, defined as 100 * beta_tor * a[m] * B0 [T] / ip [MA]
1 |
global_quantities/beta_pol(:) ⇹1FLT_1D¶Poloidal beta. […]
Poloidal beta. Defined as betap = 4 int(p dV) / [R_0 * mu_0 * Ip^2]
1 |
global_quantities/energy_diamagnetic(:) ⇹JFLT_1D¶Plasma energy content = 3/2 \* integral over the plasma volume […]
Plasma energy content = 3/2 * integral over the plasma volume of the total perpendicular pressure
1 |
global_quantities/z_eff_resistive(:) ⇹1FLT_1D¶Volume average plasma effective charge, estimated from the flux […]
Volume average plasma effective charge, estimated from the flux consumption in the ohmic phase
1 |
global_quantities/t_e_peaking(:) ⇹1FLT_1D¶Electron temperature peaking factor, defined as the Te value […]
Electron temperature peaking factor, defined as the Te value at the magnetic axis divided by the volume averaged Te (average over the plasma volume up to the LCFS)
1 |
global_quantities/t_i_average_peaking(:) ⇹1FLT_1D¶Ion temperature (averaged over ion species and states) peaking […]
Ion temperature (averaged over ion species and states) peaking factor, defined as the Ti value at the magnetic axis divided by the volume averaged Ti (average over the plasma volume up to the LCFS)
1 |
global_quantities/resistive_psi_losses(:) ⇹WbFLT_1D¶Resistive part of the poloidal flux losses, defined as the volume-averaged […]
Resistive part of the poloidal flux losses, defined as the volume-averaged scalar product of the electric field and the ohmic current density, normalized by the plasma current and integrated in time from the beginning of the plasma discharge: int ( (int(E_field_tor.j_ohm_tor) dV) / Ip ) dt)
1 |
global_quantities/ejima(:) ⇹1FLT_1D¶Ejima coefficient : resistive psi losses divided by (mu0\*R\*Ip). […]
Ejima coefficient : resistive psi losses divided by (mu0*R*Ip). See S. Ejima et al, Nuclear Fusion, Vol.22, No.10 (1982), 1313
1 |
global_quantities/t_e_volume_average(:) ⇹eVFLT_1D¶Volume averaged electron temperature (average over the plasma […]
Volume averaged electron temperature (average over the plasma volume up to the LCFS)
1 |
New in version >3.33.0.
global_quantities/n_e_volume_average(:) ⇹m^-3FLT_1D¶Volume averaged electron density (average over the plasma volume […]
Volume averaged electron density (average over the plasma volume up to the LCFS)
1 |
New in version >3.33.0.
global_quantities/ion(i1)AoS¶Quantities related to the different ion species, in the sense […]
Quantities related to the different ion species, in the sense of isonuclear or isomolecular sequences. The set of ion species of this array must be the same as the one defined in profiles_1d/ion, at the time slice indicated in ion_time_slice
Maximum occurrences (MDS+ backend only): 20
1 |
New in version >3.33.0.
global_quantities/ion(i1)/t_i_volume_average(:) ⇹eVFLT_1D¶Volume averaged temperature of this ion species (averaged over […]
Volume averaged temperature of this ion species (averaged over the plasma volume up to the LCFS)
1 |
vacuum_toroidal_fieldstructure¶Characteristics of the vacuum toroidal field (used in rho_tor […]
Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities)
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)
covariancestructure¶User defined covariance matrix. […]
User defined covariance matrix. The covariance of various quantities can be stored here, these quantities are referred to by giving their IDS path in the rows_uri list
New in version 3.40.0: lifecycle status alpha
New in version >3.39.0.
covariance/descriptionSTR_0D¶Description of this covariance matrix
Description of this covariance matrix
covariance/rows_uri(:)STR_1D¶List of URIs corresponding to the rows (1st dimension) of the […]
List of URIs corresponding to the rows (1st dimension) of the covariance matrix. If not all indices of a given node are used, they must be listed explicitly e.g. rows_uri(i) = pf_active:1/coil(i) will refer to a list of indices of the occurrence 1 of the pf_active IDS of this data entry. If the rows correspond to all indices of a given vector it is sufficient to give a single URI where this vector is denoted using the (:) implicit notation, e.g. rows_uri(1) = /grid_ggd(3)/grid_subset(2)/elements(:).
Click here for further documentation.
1 |
|
statistics(itime)AoS¶Statistics for various time slices
Statistics for various time slices
1 |
New in version 3.40.0: lifecycle status alpha
New in version >3.39.0.
statistics(itime)/quantity_2d(i1)AoS¶Set of 2D quantities on which statistics are provided. […]
Set of 2D quantities on which statistics are provided. 2D means 1D+time dimension, so either a 1D quantity within a dynamic array of structure, or a 2D dynamic quantity outside of an array of structure. Therefore the resulting statistical value is 1D for a given statistics time slice.
1 |
|
statistics(itime)/quantity_2d(i1)/pathSTR_0D¶Path of the quantity within the IDS, following the syntax given […]
Path of the quantity within the IDS, following the syntax given in the link below
statistics(itime)/quantity_2d(i1)/statistics_type(i2)AoS¶Set of statistics types applied to the quantity
Set of statistics types applied to the quantity
1 |
|
statistics(itime)/quantity_2d(i1)/statistics_type(i2)/identifierstructure¶Identifier of the statistics type
Identifier of the statistics type
This is an identifier. See statistics_type_identifier
for the available options.
statistics(itime)/quantity_2d(i1)/statistics_type(i2)/identifier/nameSTR_0D¶Short string identifier
Short string identifier
statistics(itime)/quantity_2d(i1)/statistics_type(i2)/value(:) ⇹mixedFLT_1D¶Value of the statistics for that quantity, the array corresponding […]
Value of the statistics for that quantity, the array corresponding to the first dimension of the original 2D quantity
1 |
|
statistics(itime)/quantity_2d(i1)/statistics_type(i2)/grid_subset_indexINT_0D¶Only if the statistics value is given on a different GGD grid […]
Only if the statistics value is given on a different GGD grid subset than the original quantity (e.g. if the statistics has worked over a dimension of the GGD), index of the new grid subset the statistics value is provided on. Corresponds to the index used in the grid subset definition: grid_subset(:)/identifier/index
statistics(itime)/quantity_2d(i1)/statistics_type(i2)/grid_indexINT_0D¶Only if the statistics value is given on a different GGD grid […]
Only if the statistics value is given on a different GGD grid subset than the original quantity (e.g. if the statistics has worked over a dimension of the GGD), index of the grid used to represent the statistics value
statistics(itime)/quantity_2d(i1)/distributionstructure¶Probability distribution function of the quantity
Probability distribution function of the quantity
statistics(itime)/quantity_2d(i1)/distribution/bins(:,:) ⇹mixedFLT_2D¶Bins of quantitiy values, defined for each element (first dimension) […]
Bins of quantitiy values, defined for each element (first dimension) corresponding to the first dimension of the original 2D quantity
1 |
|
2 |
|
statistics(itime)/quantity_2d(i1)/distribution/probability(:,:) ⇹1FLT_2D¶Probability to have a value of the quantity between bins(n) and […]
Probability to have a value of the quantity between bins(n) and bins(n+1) (thus the size of its second dimension is the size of the second dimension of the bins array - 1). The first dimension correspond to the first dimension of the original 2D quantity
1 |
|
2 |
|
statistics(itime)/uq_input_2d(i1)AoS¶If the statistics are based on an uncertainty quantification […]
If the statistics are based on an uncertainty quantification process, set of 2D input quantities that are varied
1 |
|
statistics(itime)/uq_input_2d(i1)/pathSTR_0D¶Path of the quantity within the IDS, following the syntax given […]
Path of the quantity within the IDS, following the syntax given in the link below
statistics(itime)/uq_input_2d(i1)/distributionstructure¶Probability distribution function of the quantity
Probability distribution function of the quantity
statistics(itime)/uq_input_2d(i1)/distribution/bins(:,:) ⇹mixedFLT_2D¶Bins of quantitiy values, defined for each element (first dimension) […]
Bins of quantitiy values, defined for each element (first dimension) corresponding to the first dimension of the original 2D quantity
1 |
|
2 |
|
statistics(itime)/uq_input_2d(i1)/distribution/probability(:,:) ⇹1FLT_2D¶Probability to have a value of the quantity between bins(n) and […]
Probability to have a value of the quantity between bins(n) and bins(n+1) (thus the size of its second dimension is the size of the second dimension of the bins array - 1). The first dimension correspond to the first dimension of the original 2D quantity
1 |
|
2 |
|