Notation of array of structure indices: itime indicates a time index; i1, i2, i3,
... indicate other indices with their depth in the IDS. This notation clarifies the
path of a given node, but should not be used to compare indices of different nodes
(they may have different meanings).
Full path name |
Description |
Data Type |
Coordinates |
ids_properties |
Interface Data Structure properties. This element identifies the node above as an
IDS |
structure |
|
ids_properties/comment |
Any comment describing the content of this IDS {constant} |
STR_0D |
|
ids_properties/name |
User-defined name for this IDS occurrence {constant}. Introduced after DD version 3.39.0 |
STR_0D |
|
ids_properties/homogeneous_time |
This node must be filled (with 0, 1, or 2) for the IDS to be valid. If 1, the time
of this IDS is homogeneous, i.e. the time values for this IDS are stored in the time
node just below the root of this IDS. If 0, the time values are stored in the various
time fields at lower levels in the tree. In the case only constant or static nodes
are filled within the IDS, homogeneous_time must be set to 2 {constant} |
INT_0D |
|
ids_properties/occurrence_type |
Type of data contained in this occurrence. Introduced after DD version 3.39.0. Available options (refer to the children of this identifier structure) :
Name |
Index |
Description |
reconstruction |
1 |
Equilibrium reconstruction |
prediction_fixed |
2 |
Equilibrium prediction, fixed boundary |
prediction_free |
3 |
Equilibrium prediction, free boundary |
mapping |
4 |
Used for mapping equilibrium results from one grid type / resolution to another, or
for including variables not present in the first set such as the calculation of magnetic
field of other derived parameters |
|
structure |
|
ids_properties/occurrence_type/name |
Short string identifier {constant} |
STR_0D |
|
ids_properties/occurrence_type/index |
Integer identifier (enumeration index within a list). Private identifier values must
be indicated by a negative index. {constant} |
INT_0D |
|
ids_properties/occurrence_type/description |
Verbose description {constant} |
STR_0D |
|
ids_properties/provider |
Name of the person in charge of producing this data {constant} |
STR_0D |
|
ids_properties/creation_date |
Date at which this data has been produced {constant} |
STR_0D |
|
ids_properties/version_put |
Version of the access layer package used to PUT this IDS |
structure |
|
ids_properties/version_put/data_dictionary |
Version of Data Dictionary used to PUT this IDS {constant} |
STR_0D |
|
ids_properties/version_put/access_layer |
Version of Access Layer used to PUT this IDS {constant} |
STR_0D |
|
ids_properties/version_put/access_layer_language |
Programming language of the Access Layer high level API used to PUT this IDS {constant} |
STR_0D |
|
ids_properties/provenance Lifecycle status: alpha since version 3.34.0 |
Provenance information about this IDS |
structure |
|
ids_properties/provenance/node(i1) |
Set of IDS nodes for which the provenance is given. The provenance information applies
to the whole structure below the IDS node. For documenting provenance information
for the whole IDS, set the size of this array of structure to 1 and leave the child
"path" node empty {constant} |
array of structures [max_size=20 (limited in MDS+ backend only)] |
1- 1...N
|
ids_properties/provenance/node(i1)/path |
Path of the node within the IDS, following the syntax given in the link below. If
empty, means the provenance information applies to the whole IDS. Click here for further documentation. {constant} |
STR_0D |
|
ids_properties/provenance/node(i1)/reference(i2) |
List of references used to populate or calculate this node, identified as explained
below. In case the node is the result of of a calculation / data processing, the reference
is an input to the process described in the "code" structure at the root of the IDS.
The reference can be an IDS (identified by a URI or a persitent identifier, see syntax
in the link below) or non-IDS data imported directly from an non-IMAS database (identified
by the command used to import the reference, or the persistent identifier of the data
reference). Often data are obtained by a chain of processes, however only the last
process input are recorded here. The full chain of provenance has then to be reconstructed
recursively from the provenance information contained in the data references. Click here for further documentation.. Introduced after DD version 3.41.0 |
array of structures [max_size=10 (limited in MDS+ backend only)] |
1- 1...N
|
ids_properties/provenance/node(i1)/reference(i2)/name |
Reference name {constant} |
STR_0D |
|
ids_properties/provenance/node(i1)/reference(i2)/timestamp |
Date and time (UTC) at which the reference was created, expressed in a human readable
form (ISO 8601) : the format of the string shall be : YYYY-MM-DDTHH:MM:SSZ. Example
: 2020-07-24T14:19:00Z {constant} |
STR_0D |
|
ids_properties/plugins Lifecycle status: alpha since version 3.39.0 |
Information about the plugins used to write/read this IDS. This structure is filled
automatically by the Access Layer at GET/PUT time, no need to fill it via a user program.. Introduced after DD version 3.38.1 |
structure |
|
ids_properties/plugins/node(i1) |
Set of IDS nodes for which a plugin has been applied {constant} |
array of structures [max_size=20 (limited in MDS+ backend only)] |
1- 1...N
|
ids_properties/plugins/node(i1)/path |
Path of the node within the IDS, following the syntax given in the link below. If
empty, means the plugin applies to the whole IDS. Click here for further documentation. {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/put_operation(i2) |
Plugins used to PUT a node (potentially, multiple plugins can be applied, if so they
are listed by order of application) |
array of structures [max_size=10 (limited in MDS+ backend only)] |
1- 1...N
|
ids_properties/plugins/node(i1)/put_operation(i2)/name |
Name of software used {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/put_operation(i2)/description |
Short description of the software (type, purpose) {constant}. Introduced after DD version 3.38.1 |
STR_0D |
|
ids_properties/plugins/node(i1)/put_operation(i2)/commit |
Unique commit reference of software {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/put_operation(i2)/version |
Unique version (tag) of software {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/put_operation(i2)/repository |
URL of software repository {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/put_operation(i2)/parameters |
List of the code specific parameters in XML format {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/readback(i2) |
Plugins to be used to read back a node (potentially, multiple plugins can be applied,
listed in reverse order of application) |
array of structures [max_size=10 (limited in MDS+ backend only)] |
1- 1...N
|
ids_properties/plugins/node(i1)/readback(i2)/name |
Name of software used {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/readback(i2)/description |
Short description of the software (type, purpose) {constant}. Introduced after DD version 3.38.1 |
STR_0D |
|
ids_properties/plugins/node(i1)/readback(i2)/commit |
Unique commit reference of software {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/readback(i2)/version |
Unique version (tag) of software {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/readback(i2)/repository |
URL of software repository {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/readback(i2)/parameters |
List of the code specific parameters in XML format {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/get_operation(i2) |
Plugins actually used to read back a node (potentially, multiple plugins can be applied,
listed in reverse order of application). This information is filled by the plugin
infrastructure during the GET operation. |
array of structures [max_size=10 (limited in MDS+ backend only)] |
1- 1...N
|
ids_properties/plugins/node(i1)/get_operation(i2)/name |
Name of software used {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/get_operation(i2)/description |
Short description of the software (type, purpose) {constant}. Introduced after DD version 3.38.1 |
STR_0D |
|
ids_properties/plugins/node(i1)/get_operation(i2)/commit |
Unique commit reference of software {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/get_operation(i2)/version |
Unique version (tag) of software {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/get_operation(i2)/repository |
URL of software repository {constant} |
STR_0D |
|
ids_properties/plugins/node(i1)/get_operation(i2)/parameters |
List of the code specific parameters in XML format {constant} |
STR_0D |
|
ids_properties/plugins/infrastructure_put |
Plugin infrastructure used to PUT the data |
structure |
|
ids_properties/plugins/infrastructure_put/name |
Name of software used {constant} |
STR_0D |
|
ids_properties/plugins/infrastructure_put/description |
Short description of the software (type, purpose) {constant}. Introduced after DD version 3.38.1 |
STR_0D |
|
ids_properties/plugins/infrastructure_put/commit |
Unique commit reference of software {constant} |
STR_0D |
|
ids_properties/plugins/infrastructure_put/version |
Unique version (tag) of software {constant} |
STR_0D |
|
ids_properties/plugins/infrastructure_put/repository |
URL of software repository {constant} |
STR_0D |
|
ids_properties/plugins/infrastructure_get |
Plugin infrastructure used to GET the data |
structure |
|
ids_properties/plugins/infrastructure_get/name |
Name of software used {constant} |
STR_0D |
|
ids_properties/plugins/infrastructure_get/description |
Short description of the software (type, purpose) {constant}. Introduced after DD version 3.38.1 |
STR_0D |
|
ids_properties/plugins/infrastructure_get/commit |
Unique commit reference of software {constant} |
STR_0D |
|
ids_properties/plugins/infrastructure_get/version |
Unique version (tag) of software {constant} |
STR_0D |
|
ids_properties/plugins/infrastructure_get/repository |
URL of software repository {constant} |
STR_0D |
|
model_type |
Type of model used to populate this IDS. Available options (refer to the children of this identifier structure) :
Name |
Index |
Description |
global |
1 |
Global calculation |
local |
2 |
Local calculation |
analytical |
3 |
Analytical estimate |
|
structure |
|
model_type/name |
Short string identifier {constant} |
STR_0D |
|
model_type/index |
Integer identifier (enumeration index within a list). Private identifier values must
be indicated by a negative index. {constant} |
INT_0D |
|
model_type/description |
Verbose description {constant} |
STR_0D |
|
equations |
Type of MHD equations used to populate this IDS. Available options (refer to the children of this identifier structure) :
Name |
Index |
Description |
reduced |
1 |
Reduced MHD |
reduced_kinetic |
11 |
Reduced MHD and kinetic hybrid |
full |
2 |
Full MHD |
full_kinetic |
21 |
Full MHD and kinetic hybrid |
|
structure |
|
equations/name |
Short string identifier {constant} |
STR_0D |
|
equations/index |
Integer identifier (enumeration index within a list). Private identifier values must
be indicated by a negative index. {constant} |
INT_0D |
|
equations/description |
Verbose description {constant} |
STR_0D |
|
fluids_n |
Number of fluids considered in the model {constant} |
INT_0D |
|
ideal_flag |
1 if ideal MHD is used to populate this IDS, 0 for non-ideal MHD {constant} |
INT_0D |
|
vacuum_toroidal_field |
Characteristics of the vacuum toroidal field (used in rho_tor definition and in the
normalization of current densities) |
structure |
|
vacuum_toroidal_field/r0 |
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) {constant} [m] |
FLT_0D |
|
vacuum_toroidal_field/r0_error_upper |
Upper error for "r0" {constant} [m] |
FLT_0D |
|
vacuum_toroidal_field/r0_error_lower |
Lower error for "r0" {constant} [m] |
FLT_0D |
|
vacuum_toroidal_field/b0(:) |
Vacuum toroidal field at R0 [T]; Positive sign means anti-clockwise when viewing from
above. The product R0B0 must be consistent with the b_tor_vacuum_r field of the tf
IDS. {dynamic} [T] |
FLT_1D |
1- time
|
vacuum_toroidal_field/b0_error_upper(:) |
Upper error for "b0" {dynamic} [T] |
FLT_1D |
1- time
|
vacuum_toroidal_field/b0_error_lower(:) |
Lower error for "b0" {dynamic} [T] |
FLT_1D |
1- time
|
time_slice(itime) |
Core plasma radial profiles for various time slices {dynamic} |
array of structures |
1- time_slice(itime)/time
|
time_slice(itime)/toroidal_mode(i1) |
Vector of toroidal modes. Each mode is described as exp(i(n_tor.phi - m_pol.theta
- 2.pi.frequency.t - phase)) |
array of structures |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/perturbation_type |
Type of the perturbation. Available options (refer to the children of this identifier structure) :
Name |
Index |
Description |
TAE |
1 |
Toroidal Alfven Eigenmode |
EAE |
2 |
Ellipticity-induced Alfven Eigenmode |
NAE |
3 |
Non-circular triangularity induced Alfven Eigenmode |
RSAE |
4 |
Reversed Shear Alfven Eigenmode |
BAE |
5 |
Beta induced Alfven Eigenmode |
BAAE |
6 |
Beta induced Alfven Acoustic Eigenmode |
EPM |
7 |
Energetic particle mode, outside any shear Alfven gap |
GAE |
8 |
Global Alfven Eingenmode |
GAM |
9 |
Geodesic Acoustic Mode |
EGAM |
10 |
Energetic particle-driven Geodesic Acoustic Mode |
iKINK |
11 |
Internal KINK mode |
eKINK |
12 |
External KINK mode |
Tearing |
13 |
Tearing mode |
Double_Tearing |
14 |
Double Tearing mode |
|
structure |
|
time_slice(itime)/toroidal_mode(i1)/perturbation_type/name |
Short string identifier {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/perturbation_type/index |
Integer identifier (enumeration index within a list). Private identifier values must
be indicated by a negative index. {dynamic} |
INT_0D |
|
time_slice(itime)/toroidal_mode(i1)/perturbation_type/description |
Verbose description {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/n_phi |
Toroidal mode number of the MHD mode {dynamic} |
INT_0D |
|
time_slice(itime)/toroidal_mode(i1)/m_pol_dominant |
Dominant poloidal mode number defining the mode rational surface; for TAEs the lower
of the two main m's has to be specified {dynamic} [-] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/m_pol_dominant_error_upper |
Upper error for "m_pol_dominant" {dynamic} [-] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/m_pol_dominant_error_lower |
Lower error for "m_pol_dominant" {dynamic} [-] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/ballooning_type |
Ballooning type of the mode : ballooning 0; anti-ballooning:1; flute-like:2. Available options (refer to the children of this identifier structure) :
Name |
Index |
Description |
TAE |
1 |
Toroidal Alfven Eigenmode |
EAE |
2 |
Ellipticity-induced Alfven Eigenmode |
NAE |
3 |
Non-circular triangularity induced Alfven Eigenmode |
RSAE |
4 |
Reversed Shear Alfven Eigenmode |
BAE |
5 |
Beta induced Alfven Eigenmode |
BAAE |
6 |
Beta induced Alfven Acoustic Eigenmode |
EPM |
7 |
Energetic particle mode, outside any shear Alfven gap |
GAE |
8 |
Global Alfven Eingenmode |
GAM |
9 |
Geodesic Acoustic Mode |
EGAM |
10 |
Energetic particle-driven Geodesic Acoustic Mode |
iKINK |
11 |
Internal KINK mode |
eKINK |
12 |
External KINK mode |
Tearing |
13 |
Tearing mode |
Double_Tearing |
14 |
Double Tearing mode |
|
structure |
|
time_slice(itime)/toroidal_mode(i1)/ballooning_type/name |
Short string identifier {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/ballooning_type/index |
Integer identifier (enumeration index within a list). Private identifier values must
be indicated by a negative index. {dynamic} |
INT_0D |
|
time_slice(itime)/toroidal_mode(i1)/ballooning_type/description |
Verbose description {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/radial_mode_number |
Radial mode number {dynamic} [-] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/radial_mode_number_error_upper |
Upper error for "radial_mode_number" {dynamic} [-] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/radial_mode_number_error_lower |
Lower error for "radial_mode_number" {dynamic} [-] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/growthrate |
Linear growthrate of the mode {dynamic} [Hz] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/growthrate_error_upper |
Upper error for "growthrate" {dynamic} [Hz] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/growthrate_error_lower |
Lower error for "growthrate" {dynamic} [Hz] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/frequency |
Frequency of the mode {dynamic} [Hz] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/frequency_error_upper |
Upper error for "frequency" {dynamic} [Hz] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/frequency_error_lower |
Lower error for "frequency" {dynamic} [Hz] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/phase |
Additional phase offset of mode {dynamic} [rad] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/phase_error_upper |
Upper error for "phase" {dynamic} [rad] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/phase_error_lower |
Lower error for "phase" {dynamic} [rad] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/energy_perturbed |
Perturbed energy associated to the mode {dynamic} [J] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/energy_perturbed_error_upper |
Upper error for "energy_perturbed" {dynamic} [J] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/energy_perturbed_error_lower |
Lower error for "energy_perturbed" {dynamic} [J] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/amplitude_multiplier |
Multiplier that is needed to convert the linear mode structures to the amplitude of
a non-linearly saturated mode in physical units. If empty, it means that the structures
contains no information about non-linearly saturated mode {dynamic} [mixed] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/amplitude_multiplier_error_upper |
Upper error for "amplitude_multiplier" {dynamic} [mixed] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/amplitude_multiplier_error_lower |
Lower error for "amplitude_multiplier" {dynamic} [mixed] |
FLT_0D |
|
time_slice(itime)/toroidal_mode(i1)/plasma |
MHD modes in the confined plasma |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid_type |
Selection of one of a set of grid types. Available options (refer to the children of this identifier structure) :
Name |
Index |
Description |
rectangular |
1 |
Cylindrical R,Z ala eqdsk (R=dim1, Z=dim2). In this case the position arrays should
not be filled since they are redundant with grid/dim1 and dim2. |
inverse |
2 |
Rhopolar_polar 2D polar coordinates (rho=dim1, theta=dim2) with magnetic axis as centre
of grid; the polar angle is theta= -atan2(z-zaxis,r-raxis). |
inverse_psi_straight_field_line |
11 |
Flux surface type with psi as radial label (dim1) and the straight-field line poloidal
angle (mod(index,10)=1) (dim2); could be non-equidistant; magnetic axis as centre
of grid |
inverse_psi_equal_arc |
12 |
Flux surface type with psi as radial label (dim1) and the equal arc poloidal angle
(mod(index,10)=2) (dim2) |
inverse_psi_polar |
13 |
Flux surface type with psi as radial label (dim1) and the polar poloidal angle (mod(index,10)=3)
(dim2); could be non-equidistant |
inverse_psi_straight_field_line_fourier |
14 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the straight-field
line poloidal angle (mod(index,10)=4) (dim2), could be non-equidistant; magnetic axis
as centre of grid |
inverse_psi_equal_arc_fourier |
15 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the equal arc
poloidal angle (mod(index,10)=5) (dim2) |
inverse_psi_polar_fourier |
16 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the polar poloidal
angle (mod(index,10)=6) (dim2); could be non-equidistant |
inverse_rhopolnorm_straight_field_line |
21 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the straight-field line poloidal angle (dim2) |
inverse_rhopolnorm_equal_arc |
22 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the equal arc poloidal angle (dim2) |
inverse_rhopolnorm_polar |
23 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the polar poloidal angle (dim2) |
inverse_rhopolnorm_straight_field_line_fourier |
24 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the straight-field line poloidal angle (dim2) |
inverse_rhopolnorm_equal_arc_fourier |
25 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the equal arc poloidal angle (dim2) |
inverse_rhopolnorm_polar_fourier |
26 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the polar poloidal angle (dim2) |
inverse_rhotornorm_straight_field_line |
31 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the straight-field
line poloidal angle (dim2) |
inverse_rhotornorm_equal_arc |
32 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the equal arc poloidal
angle (dim2) |
inverse_rhotornorm_polar |
33 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the polar poloidal
angle (dim2) |
inverse_rhotornorm_straight_field_line_fourier |
34 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the straight-field line poloidal angle (dim2) |
inverse_rhotornorm_equal_arc_fourier |
35 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the equal arc poloidal angle (dim2) |
inverse_rhotornorm_polar_fourier |
36 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the polar poloidal angle (dim2) |
inverse_rhopol_straight_field_line |
41 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the straight-field
line poloidal angle (dim2) |
inverse_rhopol_equal_arc |
42 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the equal arc poloidal
angle (dim2) |
inverse_rhopol_polar |
43 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the polar poloidal
angle (dim2) |
inverse_rhopol_straight_field_line_fourier |
44 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the straight-field line poloidal angle (dim2) |
inverse_rhopol_equal_arc_fourier |
45 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the equal arc poloidal angle (dim2) |
inverse_rhopol_polar_fourier |
46 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the polar poloidal angle (dim2) |
inverse_rhotor_straight_field_line |
51 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the straight-field line poloidal angle (dim2) |
inverse_rhotor_equal_arc |
52 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the equal arc poloidal angle (dim2) |
inverse_rhotor_polar |
53 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the polar poloidal angle (dim2) |
inverse_rhotor_straight_field_line_fourier |
54 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the straight-field line poloidal angle (dim2) |
inverse_rhotor_equal_arc_fourier |
55 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the equal arc poloidal angle (dim2) |
inverse_rhotor_polar_fourier |
56 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the polar poloidal angle (dim2) |
irregular_rz_na |
91 |
Irregular grid, thus give list of vertices in dim1(1:ndim1), dim2(1:ndim1) and then
all fields are on values(1:ndim1,1) |
|
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid_type/name |
Short string identifier {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid_type/index |
Integer identifier (enumeration index within a list). Private identifier values must
be indicated by a negative index. {dynamic} |
INT_0D |
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid_type/description |
Verbose description {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid |
Definition of the 2D grid (the content of dim1 and dim2 is defined by the selected
grid_type) |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1(:) |
First dimension values {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1_error_upper(:) |
Upper error for "dim1" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1_error_lower(:) |
Lower error for "dim1" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2(:) |
Second dimension values {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2_error_upper(:) |
Upper error for "dim2" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2_error_lower(:) |
Lower error for "dim2" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid/volume_element(:,:) |
Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i)
dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)] {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid/volume_element_error_upper(:,:) |
Upper error for "volume_element" {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/grid/volume_element_error_lower(:,:) |
Lower error for "volume_element" {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system |
Flux surface coordinate system of the equilibrium used for the MHD calculation on
a square grid of flux and poloidal angle |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid_type |
Selection of one of a set of grid types. Available options (refer to the children of this identifier structure) :
Name |
Index |
Description |
rectangular |
1 |
Cylindrical R,Z ala eqdsk (R=dim1, Z=dim2). In this case the position arrays should
not be filled since they are redundant with grid/dim1 and dim2. |
inverse |
2 |
Rhopolar_polar 2D polar coordinates (rho=dim1, theta=dim2) with magnetic axis as centre
of grid; the polar angle is theta= -atan2(z-zaxis,r-raxis). |
inverse_psi_straight_field_line |
11 |
Flux surface type with psi as radial label (dim1) and the straight-field line poloidal
angle (mod(index,10)=1) (dim2); could be non-equidistant; magnetic axis as centre
of grid |
inverse_psi_equal_arc |
12 |
Flux surface type with psi as radial label (dim1) and the equal arc poloidal angle
(mod(index,10)=2) (dim2) |
inverse_psi_polar |
13 |
Flux surface type with psi as radial label (dim1) and the polar poloidal angle (mod(index,10)=3)
(dim2); could be non-equidistant |
inverse_psi_straight_field_line_fourier |
14 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the straight-field
line poloidal angle (mod(index,10)=4) (dim2), could be non-equidistant; magnetic axis
as centre of grid |
inverse_psi_equal_arc_fourier |
15 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the equal arc
poloidal angle (mod(index,10)=5) (dim2) |
inverse_psi_polar_fourier |
16 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the polar poloidal
angle (mod(index,10)=6) (dim2); could be non-equidistant |
inverse_rhopolnorm_straight_field_line |
21 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the straight-field line poloidal angle (dim2) |
inverse_rhopolnorm_equal_arc |
22 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the equal arc poloidal angle (dim2) |
inverse_rhopolnorm_polar |
23 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the polar poloidal angle (dim2) |
inverse_rhopolnorm_straight_field_line_fourier |
24 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the straight-field line poloidal angle (dim2) |
inverse_rhopolnorm_equal_arc_fourier |
25 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the equal arc poloidal angle (dim2) |
inverse_rhopolnorm_polar_fourier |
26 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the polar poloidal angle (dim2) |
inverse_rhotornorm_straight_field_line |
31 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the straight-field
line poloidal angle (dim2) |
inverse_rhotornorm_equal_arc |
32 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the equal arc poloidal
angle (dim2) |
inverse_rhotornorm_polar |
33 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the polar poloidal
angle (dim2) |
inverse_rhotornorm_straight_field_line_fourier |
34 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the straight-field line poloidal angle (dim2) |
inverse_rhotornorm_equal_arc_fourier |
35 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the equal arc poloidal angle (dim2) |
inverse_rhotornorm_polar_fourier |
36 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the polar poloidal angle (dim2) |
inverse_rhopol_straight_field_line |
41 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the straight-field
line poloidal angle (dim2) |
inverse_rhopol_equal_arc |
42 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the equal arc poloidal
angle (dim2) |
inverse_rhopol_polar |
43 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the polar poloidal
angle (dim2) |
inverse_rhopol_straight_field_line_fourier |
44 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the straight-field line poloidal angle (dim2) |
inverse_rhopol_equal_arc_fourier |
45 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the equal arc poloidal angle (dim2) |
inverse_rhopol_polar_fourier |
46 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the polar poloidal angle (dim2) |
inverse_rhotor_straight_field_line |
51 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the straight-field line poloidal angle (dim2) |
inverse_rhotor_equal_arc |
52 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the equal arc poloidal angle (dim2) |
inverse_rhotor_polar |
53 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the polar poloidal angle (dim2) |
inverse_rhotor_straight_field_line_fourier |
54 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the straight-field line poloidal angle (dim2) |
inverse_rhotor_equal_arc_fourier |
55 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the equal arc poloidal angle (dim2) |
inverse_rhotor_polar_fourier |
56 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the polar poloidal angle (dim2) |
irregular_rz_na |
91 |
Irregular grid, thus give list of vertices in dim1(1:ndim1), dim2(1:ndim1) and then
all fields are on values(1:ndim1,1) |
|
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid_type/name |
Short string identifier {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid_type/index |
Integer identifier (enumeration index within a list). Private identifier values must
be indicated by a negative index. {dynamic} |
INT_0D |
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid_type/description |
Verbose description {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid |
Definition of the 2D grid |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1(:) |
First dimension values {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1_error_upper(:) |
Upper error for "dim1" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1_error_lower(:) |
Lower error for "dim1" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2(:) |
Second dimension values {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2_error_upper(:) |
Upper error for "dim2" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2_error_lower(:) |
Lower error for "dim2" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/volume_element(:,:) |
Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i)
dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)] {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/volume_element_error_upper(:,:) |
Upper error for "volume_element" {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/volume_element_error_lower(:,:) |
Lower error for "volume_element" {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/r(:,:) |
Values of the major radius on the grid {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/r_error_upper(:,:) |
Upper error for "r" {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/r_error_lower(:,:) |
Lower error for "r" {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/z(:,:) |
Values of the Height on the grid {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/z_error_upper(:,:) |
Upper error for "z" {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/z_error_lower(:,:) |
Lower error for "z" {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/jacobian(:,:) |
Absolute value of the jacobian of the coordinate system {dynamic} [mixed] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/jacobian_error_upper(:,:) |
Upper error for "jacobian" {dynamic} [mixed] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/jacobian_error_lower(:,:) |
Lower error for "jacobian" {dynamic} [mixed] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/tensor_covariant(:,:,:,:) |
Covariant metric tensor on every point of the grid described by grid_type {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/tensor_covariant_error_upper(:,:,:,:) |
Upper error for "tensor_covariant" {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/tensor_covariant_error_lower(:,:,:,:) |
Lower error for "tensor_covariant" {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/tensor_contravariant(:,:,:,:) |
Contravariant metric tensor on every point of the grid described by grid_type {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/tensor_contravariant_error_upper(:,:,:,:) |
Upper error for "tensor_contravariant" {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/tensor_contravariant_error_lower(:,:,:,:) |
Lower error for "tensor_contravariant" {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular |
Perpendicular displacement of the modes [m] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel |
Parallel displacement of the modes [m] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/tau_alfven(:) |
Alven time=R/vA=R0 sqrt(mi ni(rho))/B0 {dynamic} [s] |
FLT_1D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
|
time_slice(itime)/toroidal_mode(i1)/plasma/tau_alfven_error_upper(:) |
Upper error for "tau_alfven" {dynamic} [s] |
FLT_1D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
|
time_slice(itime)/toroidal_mode(i1)/plasma/tau_alfven_error_lower(:) |
Lower error for "tau_alfven" {dynamic} [s] |
FLT_1D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
|
time_slice(itime)/toroidal_mode(i1)/plasma/tau_resistive(:) |
Resistive time = mu_0 rho*rho/1.22/eta_neo {dynamic} [s] |
FLT_1D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
|
time_slice(itime)/toroidal_mode(i1)/plasma/tau_resistive_error_upper(:) |
Upper error for "tau_resistive" {dynamic} [s] |
FLT_1D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
|
time_slice(itime)/toroidal_mode(i1)/plasma/tau_resistive_error_lower(:) |
Lower error for "tau_resistive" {dynamic} [s] |
FLT_1D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed |
Pertubed vector potential for given toroidal mode number [T.m] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1 |
First coordinate (radial) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2 |
Second coordinate (poloidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3 |
Third coordinate (toroidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed |
Pertubed magnetic field for given toroidal mode number [T] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1 |
First coordinate (radial) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2 |
Second coordinate (poloidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3 |
Third coordinate (toroidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed |
Pertubed velocity for given toroidal mode number [m/s] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1 |
First coordinate (radial) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2 |
Second coordinate (poloidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3 |
Third coordinate (toroidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed |
Perturbed pressure for given toroidal mode number [Pa] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed |
Perturbed mass density for given toroidal mode number [kg.m^-3] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed |
Perturbed temperature for given toroidal mode number [eV] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed |
Perturbed electrostatic potential for given toroidal mode number [V] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed |
Perturbed electromagnetic super-potential for given toroidal mode number, see ref
[Antonsen/Lane Phys Fluids 23(6) 1980, formula 34], so that A_field_parallel=1/(i*2pi*frequency)
(grad psi_potential)_parallel [V] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2) |
Local shear Alfven spectrum as a function of radius (only in case grid/dim1 is a radial
coordinate) |
array of structures |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
|
time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/real(:) |
Real part of the frequency, for a given radial position and every root found at this
position {dynamic} [s^-1] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/real_error_upper(:) |
Upper error for "real" {dynamic} [s^-1] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/real_error_lower(:) |
Lower error for "real" {dynamic} [s^-1] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/imaginary(:) |
Imaginary part of the frequency, for a given radial position and every root found
at this position {dynamic} [s^-1] |
FLT_1D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/real
|
time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/imaginary_error_upper(:) |
Upper error for "imaginary" {dynamic} [s^-1] |
FLT_1D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/real
|
time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/imaginary_error_lower(:) |
Lower error for "imaginary" {dynamic} [s^-1] |
FLT_1D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/real
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwell |
Maxwell stress tensor |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwell/real(:,:,:) |
Real part of the stress tensor, for various radial positions {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwell/real_error_upper(:,:,:) |
Upper error for "real" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwell/real_error_lower(:,:,:) |
Lower error for "real" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwell/imaginary(:,:,:) |
Imaginary part of the stress tensor, for various radial positions {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwell/imaginary_error_upper(:,:,:) |
Upper error for "imaginary" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwell/imaginary_error_lower(:,:,:) |
Lower error for "imaginary" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynolds |
Reynolds stress tensor |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynolds/real(:,:,:) |
Real part of the stress tensor, for various radial positions {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynolds/real_error_upper(:,:,:) |
Upper error for "real" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynolds/real_error_lower(:,:,:) |
Lower error for "real" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynolds/imaginary(:,:,:) |
Imaginary part of the stress tensor, for various radial positions {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynolds/imaginary_error_upper(:,:,:) |
Upper error for "imaginary" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynolds/imaginary_error_lower(:,:,:) |
Lower error for "imaginary" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/ntv |
Neoclassical toroidal viscosity tensor |
structure |
|
time_slice(itime)/toroidal_mode(i1)/plasma/ntv/real(:,:,:) |
Real part of the stress tensor, for various radial positions {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/ntv/real_error_upper(:,:,:) |
Upper error for "real" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/ntv/real_error_lower(:,:,:) |
Lower error for "real" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/ntv/imaginary(:,:,:) |
Imaginary part of the stress tensor, for various radial positions {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/ntv/imaginary_error_upper(:,:,:) |
Upper error for "imaginary" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/plasma/ntv/imaginary_error_lower(:,:,:) |
Lower error for "imaginary" {dynamic} [N.m^-2] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1
2- 1...N
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum |
MHD modes in the vacuum |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid_type |
Selection of one of a set of grid types. Available options (refer to the children of this identifier structure) :
Name |
Index |
Description |
rectangular |
1 |
Cylindrical R,Z ala eqdsk (R=dim1, Z=dim2). In this case the position arrays should
not be filled since they are redundant with grid/dim1 and dim2. |
inverse |
2 |
Rhopolar_polar 2D polar coordinates (rho=dim1, theta=dim2) with magnetic axis as centre
of grid; the polar angle is theta= -atan2(z-zaxis,r-raxis). |
inverse_psi_straight_field_line |
11 |
Flux surface type with psi as radial label (dim1) and the straight-field line poloidal
angle (mod(index,10)=1) (dim2); could be non-equidistant; magnetic axis as centre
of grid |
inverse_psi_equal_arc |
12 |
Flux surface type with psi as radial label (dim1) and the equal arc poloidal angle
(mod(index,10)=2) (dim2) |
inverse_psi_polar |
13 |
Flux surface type with psi as radial label (dim1) and the polar poloidal angle (mod(index,10)=3)
(dim2); could be non-equidistant |
inverse_psi_straight_field_line_fourier |
14 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the straight-field
line poloidal angle (mod(index,10)=4) (dim2), could be non-equidistant; magnetic axis
as centre of grid |
inverse_psi_equal_arc_fourier |
15 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the equal arc
poloidal angle (mod(index,10)=5) (dim2) |
inverse_psi_polar_fourier |
16 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the polar poloidal
angle (mod(index,10)=6) (dim2); could be non-equidistant |
inverse_rhopolnorm_straight_field_line |
21 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the straight-field line poloidal angle (dim2) |
inverse_rhopolnorm_equal_arc |
22 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the equal arc poloidal angle (dim2) |
inverse_rhopolnorm_polar |
23 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the polar poloidal angle (dim2) |
inverse_rhopolnorm_straight_field_line_fourier |
24 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the straight-field line poloidal angle (dim2) |
inverse_rhopolnorm_equal_arc_fourier |
25 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the equal arc poloidal angle (dim2) |
inverse_rhopolnorm_polar_fourier |
26 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the polar poloidal angle (dim2) |
inverse_rhotornorm_straight_field_line |
31 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the straight-field
line poloidal angle (dim2) |
inverse_rhotornorm_equal_arc |
32 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the equal arc poloidal
angle (dim2) |
inverse_rhotornorm_polar |
33 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the polar poloidal
angle (dim2) |
inverse_rhotornorm_straight_field_line_fourier |
34 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the straight-field line poloidal angle (dim2) |
inverse_rhotornorm_equal_arc_fourier |
35 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the equal arc poloidal angle (dim2) |
inverse_rhotornorm_polar_fourier |
36 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the polar poloidal angle (dim2) |
inverse_rhopol_straight_field_line |
41 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the straight-field
line poloidal angle (dim2) |
inverse_rhopol_equal_arc |
42 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the equal arc poloidal
angle (dim2) |
inverse_rhopol_polar |
43 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the polar poloidal
angle (dim2) |
inverse_rhopol_straight_field_line_fourier |
44 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the straight-field line poloidal angle (dim2) |
inverse_rhopol_equal_arc_fourier |
45 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the equal arc poloidal angle (dim2) |
inverse_rhopol_polar_fourier |
46 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the polar poloidal angle (dim2) |
inverse_rhotor_straight_field_line |
51 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the straight-field line poloidal angle (dim2) |
inverse_rhotor_equal_arc |
52 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the equal arc poloidal angle (dim2) |
inverse_rhotor_polar |
53 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the polar poloidal angle (dim2) |
inverse_rhotor_straight_field_line_fourier |
54 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the straight-field line poloidal angle (dim2) |
inverse_rhotor_equal_arc_fourier |
55 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the equal arc poloidal angle (dim2) |
inverse_rhotor_polar_fourier |
56 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the polar poloidal angle (dim2) |
irregular_rz_na |
91 |
Irregular grid, thus give list of vertices in dim1(1:ndim1), dim2(1:ndim1) and then
all fields are on values(1:ndim1,1) |
|
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid_type/name |
Short string identifier {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid_type/index |
Integer identifier (enumeration index within a list). Private identifier values must
be indicated by a negative index. {dynamic} |
INT_0D |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid_type/description |
Verbose description {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid |
Definition of the 2D grid (the content of dim1 and dim2 is defined by the selected
grid_type) |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1(:) |
First dimension values {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1_error_upper(:) |
Upper error for "dim1" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1_error_lower(:) |
Lower error for "dim1" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2(:) |
Second dimension values {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2_error_upper(:) |
Upper error for "dim2" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2_error_lower(:) |
Lower error for "dim2" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/volume_element(:,:) |
Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i)
dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)] {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/volume_element_error_upper(:,:) |
Upper error for "volume_element" {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/volume_element_error_lower(:,:) |
Lower error for "volume_element" {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system |
Flux surface coordinate system of the equilibrium used for the MHD calculation on
a square grid of flux and poloidal angle |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid_type |
Selection of one of a set of grid types. Available options (refer to the children of this identifier structure) :
Name |
Index |
Description |
rectangular |
1 |
Cylindrical R,Z ala eqdsk (R=dim1, Z=dim2). In this case the position arrays should
not be filled since they are redundant with grid/dim1 and dim2. |
inverse |
2 |
Rhopolar_polar 2D polar coordinates (rho=dim1, theta=dim2) with magnetic axis as centre
of grid; the polar angle is theta= -atan2(z-zaxis,r-raxis). |
inverse_psi_straight_field_line |
11 |
Flux surface type with psi as radial label (dim1) and the straight-field line poloidal
angle (mod(index,10)=1) (dim2); could be non-equidistant; magnetic axis as centre
of grid |
inverse_psi_equal_arc |
12 |
Flux surface type with psi as radial label (dim1) and the equal arc poloidal angle
(mod(index,10)=2) (dim2) |
inverse_psi_polar |
13 |
Flux surface type with psi as radial label (dim1) and the polar poloidal angle (mod(index,10)=3)
(dim2); could be non-equidistant |
inverse_psi_straight_field_line_fourier |
14 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the straight-field
line poloidal angle (mod(index,10)=4) (dim2), could be non-equidistant; magnetic axis
as centre of grid |
inverse_psi_equal_arc_fourier |
15 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the equal arc
poloidal angle (mod(index,10)=5) (dim2) |
inverse_psi_polar_fourier |
16 |
Flux surface type with psi as radial label (dim1) and Fourier modes in the polar poloidal
angle (mod(index,10)=6) (dim2); could be non-equidistant |
inverse_rhopolnorm_straight_field_line |
21 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the straight-field line poloidal angle (dim2) |
inverse_rhopolnorm_equal_arc |
22 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the equal arc poloidal angle (dim2) |
inverse_rhopolnorm_polar |
23 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and the polar poloidal angle (dim2) |
inverse_rhopolnorm_straight_field_line_fourier |
24 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the straight-field line poloidal angle (dim2) |
inverse_rhopolnorm_equal_arc_fourier |
25 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the equal arc poloidal angle (dim2) |
inverse_rhopolnorm_polar_fourier |
26 |
Flux surface type with radial label sqrt[(psi-psi_axis)/(psi_edge-psi_axis)] (dim1)
and Fourier modes in the polar poloidal angle (dim2) |
inverse_rhotornorm_straight_field_line |
31 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the straight-field
line poloidal angle (dim2) |
inverse_rhotornorm_equal_arc |
32 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the equal arc poloidal
angle (dim2) |
inverse_rhotornorm_polar |
33 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and the polar poloidal
angle (dim2) |
inverse_rhotornorm_straight_field_line_fourier |
34 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the straight-field line poloidal angle (dim2) |
inverse_rhotornorm_equal_arc_fourier |
35 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the equal arc poloidal angle (dim2) |
inverse_rhotornorm_polar_fourier |
36 |
Flux surface type with radial label sqrt[Phi/Phi_edge] (dim1) and Fourier modes in
the polar poloidal angle (dim2) |
inverse_rhopol_straight_field_line |
41 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the straight-field
line poloidal angle (dim2) |
inverse_rhopol_equal_arc |
42 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the equal arc poloidal
angle (dim2) |
inverse_rhopol_polar |
43 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and the polar poloidal
angle (dim2) |
inverse_rhopol_straight_field_line_fourier |
44 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the straight-field line poloidal angle (dim2) |
inverse_rhopol_equal_arc_fourier |
45 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the equal arc poloidal angle (dim2) |
inverse_rhopol_polar_fourier |
46 |
Flux surface type with radial label sqrt[psi-psi_axis] (dim1) and Fourier modes in
the polar poloidal angle (dim2) |
inverse_rhotor_straight_field_line |
51 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the straight-field line poloidal angle (dim2) |
inverse_rhotor_equal_arc |
52 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the equal arc poloidal angle (dim2) |
inverse_rhotor_polar |
53 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and the polar poloidal angle (dim2) |
inverse_rhotor_straight_field_line_fourier |
54 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the straight-field line poloidal angle (dim2) |
inverse_rhotor_equal_arc_fourier |
55 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the equal arc poloidal angle (dim2) |
inverse_rhotor_polar_fourier |
56 |
Flux surface type with radial label sqrt[Phi/pi/B0] (dim1), Phi being toroidal flux,
and Fourier modes in the polar poloidal angle (dim2) |
irregular_rz_na |
91 |
Irregular grid, thus give list of vertices in dim1(1:ndim1), dim2(1:ndim1) and then
all fields are on values(1:ndim1,1) |
|
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid_type/name |
Short string identifier {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid_type/index |
Integer identifier (enumeration index within a list). Private identifier values must
be indicated by a negative index. {dynamic} |
INT_0D |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid_type/description |
Verbose description {dynamic} |
STR_0D |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid |
Definition of the 2D grid |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1(:) |
First dimension values {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1_error_upper(:) |
Upper error for "dim1" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1_error_lower(:) |
Lower error for "dim1" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2(:) |
Second dimension values {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2_error_upper(:) |
Upper error for "dim2" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2_error_lower(:) |
Lower error for "dim2" {dynamic} [mixed] |
FLT_1D |
1- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/volume_element(:,:) |
Elementary plasma volume of plasma enclosed in the cell formed by the nodes [dim1(i)
dim2(j)], [dim1(i+1) dim2(j)], [dim1(i) dim2(j+1)] and [dim1(i+1) dim2(j+1)] {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/volume_element_error_upper(:,:) |
Upper error for "volume_element" {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/volume_element_error_lower(:,:) |
Lower error for "volume_element" {dynamic} [m^3] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/r(:,:) |
Values of the major radius on the grid {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/r_error_upper(:,:) |
Upper error for "r" {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/r_error_lower(:,:) |
Lower error for "r" {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/z(:,:) |
Values of the Height on the grid {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/z_error_upper(:,:) |
Upper error for "z" {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/z_error_lower(:,:) |
Lower error for "z" {dynamic} [m] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/jacobian(:,:) |
Absolute value of the jacobian of the coordinate system {dynamic} [mixed] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/jacobian_error_upper(:,:) |
Upper error for "jacobian" {dynamic} [mixed] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/jacobian_error_lower(:,:) |
Lower error for "jacobian" {dynamic} [mixed] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/tensor_covariant(:,:,:,:) |
Covariant metric tensor on every point of the grid described by grid_type {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/tensor_covariant_error_upper(:,:,:,:) |
Upper error for "tensor_covariant" {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/tensor_covariant_error_lower(:,:,:,:) |
Lower error for "tensor_covariant" {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/tensor_contravariant(:,:,:,:) |
Contravariant metric tensor on every point of the grid described by grid_type {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/tensor_contravariant_error_upper(:,:,:,:) |
Upper error for "tensor_contravariant" {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/tensor_contravariant_error_lower(:,:,:,:) |
Lower error for "tensor_contravariant" {dynamic} [mixed] |
FLT_4D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2
3- 1...3
4- 1...3
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed |
Pertubed vector potential for given toroidal mode number [T.m] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1 |
First coordinate (radial) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2 |
Second coordinate (poloidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3 |
Third coordinate (toroidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed |
Pertubed magnetic field for given toroidal mode number [T] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1 |
First coordinate (radial) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2 |
Second coordinate (poloidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3 |
Third coordinate (toroidal) [as_parent] |
structure |
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/real(:,:) |
Real part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/real_error_upper(:,:) |
Upper error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/real_error_lower(:,:) |
Lower error for "real" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/imaginary(:,:) |
Imaginary part {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/imaginary_error_upper(:,:) |
Upper error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/imaginary_error_lower(:,:) |
Lower error for "imaginary" {dynamic} [as_parent] |
FLT_2D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/coefficients_real(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (real part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/coefficients_real_error_upper(:,:,:) |
Upper error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/coefficients_real_error_lower(:,:,:) |
Lower error for "coefficients_real" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/coefficients_imaginary(:,:,:) |
Interpolation coefficients, to be used for a high precision evaluation of the physical
quantity (imaginary part) with finite elements, provided on the 2D grid {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/coefficients_imaginary_error_upper(:,:,:) |
Upper error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/coefficients_imaginary_error_lower(:,:,:) |
Lower error for "coefficients_imaginary" {dynamic} [as_parent] |
FLT_3D |
1- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1
2- time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2
3- 1...N
|
time_slice(itime)/time |
Time {dynamic} [s] |
FLT_0D |
|
code |
Generic decription of the code-specific parameters for the code that has produced
this IDS |
structure |
|
code/name |
Name of software generating IDS {constant} |
STR_0D |
|
code/description |
Short description of the software (type, purpose) {constant}. Introduced after DD version 3.38.1 |
STR_0D |
|
code/commit |
Unique commit reference of software {constant} |
STR_0D |
|
code/version |
Unique version (tag) of software {constant} |
STR_0D |
|
code/repository |
URL of software repository {constant} |
STR_0D |
|
code/parameters |
List of the code specific parameters in XML format {constant} |
STR_0D |
|
code/output_flag(:) |
Output flag : 0 means the run is successful, other values mean some difficulty has
been encountered, the exact meaning is then code specific. Negative values mean the
result shall not be used. {dynamic} |
INT_1D |
1- time
|
code/library(i1) |
List of external libraries used by the code that has produced this IDS |
array of structures [max_size=10 (limited in MDS+ backend only)] |
1- 1...N
|
code/library(i1)/name |
Name of software {constant} |
STR_0D |
|
code/library(i1)/description |
Short description of the software (type, purpose) {constant}. Introduced after DD version 3.38.1 |
STR_0D |
|
code/library(i1)/commit |
Unique commit reference of software {constant} |
STR_0D |
|
code/library(i1)/version |
Unique version (tag) of software {constant} |
STR_0D |
|
code/library(i1)/repository |
URL of software repository {constant} |
STR_0D |
|
code/library(i1)/parameters |
List of the code specific parameters in XML format {constant} |
STR_0D |
|
time(:) |
Generic time {dynamic} [s] |
FLT_1D |
1- 1...N
|