mhd_linear¶
Magnetohydronamic linear stability
Maximum occurrences (MDS+ backend only): 10
New in version 3.0.4: lifecycle status alpha
Changed in version 3.30.0.
ids_propertiesstructure¶
See common IDS structure reference: ids_properties.
model_typestructure¶Type of model used to populate this IDS
Type of model used to populate this IDS
This is an identifier. See mhd_linear_model_identifier for the available options.
equationsstructure¶Type of MHD equations used to populate this IDS
Type of MHD equations used to populate this IDS
This is an identifier. See mhd_linear_equations_identifier for the available options.
ideal_flagINT_0D¶1 if ideal MHD is used to populate this IDS, 0 for non-ideal […]
1 if ideal MHD is used to populate this IDS, 0 for non-ideal MHD
vacuum_toroidal_fieldstructure¶Characteristics of the vacuum toroidal field (used in rho_tor […]
Characteristics of the vacuum toroidal field (used in rho_tor definition and in the normalization of current densities)
vacuum_toroidal_field/r0 ⇹mFLT_0D¶Reference major radius where the vacuum toroidal magnetic field […]
Reference major radius where the vacuum toroidal magnetic field is given (usually a fixed position such as the middle of the vessel at the equatorial midplane)
time_slice(itime)AoS¶Core plasma radial profiles for various time slices
Core plasma radial profiles for various time slices
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time_slice(itime)/toroidal_mode(i1)AoS¶Vector of toroidal modes. […]
Vector of toroidal modes. Each mode is described as exp(i(n_tor.phi - m_pol.theta - 2.pi.frequency.t - phase))
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time_slice(itime)/toroidal_mode(i1)/perturbation_typestructure¶Type of the perturbation
Type of the perturbation
This is an identifier. See mhd_linear_perturbation_identifier for the available options.
time_slice(itime)/toroidal_mode(i1)/perturbation_type/nameSTR_0D¶Short string identifier
Short string identifier
time_slice(itime)/toroidal_mode(i1)/n_phiINT_0D¶Toroidal mode number of the MHD mode
Toroidal mode number of the MHD mode
Changed in version 3.42.0: Renamed from n_tor
time_slice(itime)/toroidal_mode(i1)/m_pol_dominant ⇹1FLT_0D¶Dominant poloidal mode number defining the mode rational surface; […]
Dominant poloidal mode number defining the mode rational surface; for TAEs the lower of the two main m’s has to be specified
time_slice(itime)/toroidal_mode(i1)/ballooning_typestructure¶Ballooning type of the mode : ballooning 0; anti-ballooning:1; […]
Ballooning type of the mode : ballooning 0; anti-ballooning:1; flute-like:2
This is an identifier. See mhd_linear_perturbation_identifier for the available options.
time_slice(itime)/toroidal_mode(i1)/ballooning_type/nameSTR_0D¶Short string identifier
Short string identifier
time_slice(itime)/toroidal_mode(i1)/radial_mode_number ⇹1FLT_0D¶Radial mode number
Radial mode number
time_slice(itime)/toroidal_mode(i1)/growthrate ⇹HzFLT_0D¶Linear growthrate of the mode
Linear growthrate of the mode
time_slice(itime)/toroidal_mode(i1)/phase ⇹radFLT_0D¶Additional phase offset of mode
Additional phase offset of mode
time_slice(itime)/toroidal_mode(i1)/energy_perturbed ⇹JFLT_0D¶Perturbed energy associated to the mode
Perturbed energy associated to the mode
time_slice(itime)/toroidal_mode(i1)/amplitude_multiplier ⇹mixedFLT_0D¶Multiplier that is needed to convert the linear mode structures […]
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
time_slice(itime)/toroidal_mode(i1)/plasmastructure¶MHD modes in the confined plasma
MHD modes in the confined plasma
time_slice(itime)/toroidal_mode(i1)/plasma/grid_typestructure¶Selection of one of a set of grid types
Selection of one of a set of grid types
This is an identifier. See poloidal_plane_coordinates_identifier for the available options.
time_slice(itime)/toroidal_mode(i1)/plasma/grid_type/nameSTR_0D¶Short string identifier
Short string identifier
time_slice(itime)/toroidal_mode(i1)/plasma/gridstructure¶Definition of the 2D grid (the content of dim1 and dim2 is defined […]
Definition of the 2D grid (the content of dim1 and dim2 is defined by the selected grid_type)
time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim1(:) ⇹mixedFLT_1D¶First dimension values
First dimension values
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time_slice(itime)/toroidal_mode(i1)/plasma/grid/dim2(:) ⇹mixedFLT_1D¶Second dimension values
Second dimension values
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time_slice(itime)/toroidal_mode(i1)/plasma/grid/volume_element(:,:) ⇹m^3FLT_2D¶Elementary plasma volume of plasma enclosed in the cell formed […]
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)]
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time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_systemstructure¶Flux surface coordinate system of the equilibrium used for the […]
Flux surface coordinate system of the equilibrium used for the MHD calculation on a square grid of flux and poloidal angle
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid_typestructure¶Selection of one of a set of grid types
Selection of one of a set of grid types
This is an identifier. See poloidal_plane_coordinates_identifier for the available options.
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid_type/nameSTR_0D¶Short string identifier
Short string identifier
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/gridstructure¶Definition of the 2D grid
Definition of the 2D grid
time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim1(:) ⇹mixedFLT_1D¶First dimension values
First dimension values
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time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/dim2(:) ⇹mixedFLT_1D¶Second dimension values
Second dimension values
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time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/grid/volume_element(:,:) ⇹m^3FLT_2D¶Elementary plasma volume of plasma enclosed in the cell formed […]
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)]
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time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/r(:,:) ⇹mFLT_2D¶Values of the major radius on the grid
Values of the major radius on the grid
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time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/z(:,:) ⇹mFLT_2D¶Values of the Height on the grid
Values of the Height on the grid
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time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/jacobian(:,:) ⇹mixedFLT_2D¶Absolute value of the jacobian of the coordinate system
Absolute value of the jacobian of the coordinate system
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time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/tensor_covariant(:,:,:,:) ⇹mixedFLT_4D¶Covariant metric tensor on every point of the grid described […]
Covariant metric tensor on every point of the grid described by grid_type
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time_slice(itime)/toroidal_mode(i1)/plasma/coordinate_system/tensor_contravariant(:,:,:,:) ⇹mixedFLT_4D¶Contravariant metric tensor on every point of the grid described […]
Contravariant metric tensor on every point of the grid described by grid_type
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time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicularmstructure¶Perpendicular displacement of the modes
Perpendicular displacement of the modes
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/real(:,:) ⇹mFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/imaginary(:,:) ⇹mFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/coefficients_real(:,:,:) ⇹mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/displacement_perpendicular/coefficients_imaginary(:,:,:) ⇹mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallelmstructure¶Parallel displacement of the modes
Parallel displacement of the modes
time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/real(:,:) ⇹mFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/imaginary(:,:) ⇹mFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/coefficients_real(:,:,:) ⇹mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/displacement_parallel/coefficients_imaginary(:,:,:) ⇹mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/tau_alfven(:) ⇹sFLT_1D¶Alven time=R/vA=R0 sqrt(mi ni(rho))/B0
Alven time=R/vA=R0 sqrt(mi ni(rho))/B0
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time_slice(itime)/toroidal_mode(i1)/plasma/tau_resistive(:) ⇹sFLT_1D¶Resistive time = mu_0 rho\*rho/1.22/eta_neo
Resistive time = mu_0 rho*rho/1.22/eta_neo
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbedT.mstructure¶Pertubed vector potential for given toroidal mode number
Pertubed vector potential for given toroidal mode number
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1T.mstructure¶First coordinate (radial)
First coordinate (radial)
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/real(:,:) ⇹T.mFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/imaginary(:,:) ⇹T.mFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/coefficients_real(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate1/coefficients_imaginary(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2T.mstructure¶Second coordinate (poloidal)
Second coordinate (poloidal)
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/real(:,:) ⇹T.mFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/imaginary(:,:) ⇹T.mFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/coefficients_real(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate2/coefficients_imaginary(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3T.mstructure¶Third coordinate (toroidal)
Third coordinate (toroidal)
time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/real(:,:) ⇹T.mFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/imaginary(:,:) ⇹T.mFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/coefficients_real(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/a_field_perturbed/coordinate3/coefficients_imaginary(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbedTstructure¶Pertubed magnetic field for given toroidal mode number
Pertubed magnetic field for given toroidal mode number
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1Tstructure¶First coordinate (radial)
First coordinate (radial)
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/real(:,:) ⇹TFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/imaginary(:,:) ⇹TFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/coefficients_real(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate1/coefficients_imaginary(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2Tstructure¶Second coordinate (poloidal)
Second coordinate (poloidal)
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/real(:,:) ⇹TFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/imaginary(:,:) ⇹TFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/coefficients_real(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate2/coefficients_imaginary(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3Tstructure¶Third coordinate (toroidal)
Third coordinate (toroidal)
time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/real(:,:) ⇹TFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/imaginary(:,:) ⇹TFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/coefficients_real(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/b_field_perturbed/coordinate3/coefficients_imaginary(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbedm.s^-1structure¶Pertubed velocity for given toroidal mode number
Pertubed velocity for given toroidal mode number
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1m.s^-1structure¶First coordinate (radial)
First coordinate (radial)
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/real(:,:) ⇹m.s^-1FLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/imaginary(:,:) ⇹m.s^-1FLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/coefficients_real(:,:,:) ⇹m.s^-1FLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate1/coefficients_imaginary(:,:,:) ⇹m.s^-1FLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2m.s^-1structure¶Second coordinate (poloidal)
Second coordinate (poloidal)
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/real(:,:) ⇹m.s^-1FLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/imaginary(:,:) ⇹m.s^-1FLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/coefficients_real(:,:,:) ⇹m.s^-1FLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate2/coefficients_imaginary(:,:,:) ⇹m.s^-1FLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3m.s^-1structure¶Third coordinate (toroidal)
Third coordinate (toroidal)
time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/real(:,:) ⇹m.s^-1FLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/imaginary(:,:) ⇹m.s^-1FLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/coefficients_real(:,:,:) ⇹m.s^-1FLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/velocity_perturbed/coordinate3/coefficients_imaginary(:,:,:) ⇹m.s^-1FLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbedPastructure¶Perturbed pressure for given toroidal mode number
Perturbed pressure for given toroidal mode number
time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/real(:,:) ⇹PaFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/imaginary(:,:) ⇹PaFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/coefficients_real(:,:,:) ⇹PaFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/pressure_perturbed/coefficients_imaginary(:,:,:) ⇹PaFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbedkg.m^-3structure¶Perturbed mass density for given toroidal mode number
Perturbed mass density for given toroidal mode number
time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/real(:,:) ⇹kg.m^-3FLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/imaginary(:,:) ⇹kg.m^-3FLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/coefficients_real(:,:,:) ⇹kg.m^-3FLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/mass_density_perturbed/coefficients_imaginary(:,:,:) ⇹kg.m^-3FLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
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time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbedeVstructure¶Perturbed temperature for given toroidal mode number
Perturbed temperature for given toroidal mode number
time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/real(:,:) ⇹eVFLT_2D¶Real part
Real part
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time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/imaginary(:,:) ⇹eVFLT_2D¶Imaginary part
Imaginary part
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time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/coefficients_real(:,:,:) ⇹eVFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/temperature_perturbed/coefficients_imaginary(:,:,:) ⇹eVFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbedVstructure¶Perturbed electrostatic potential for given toroidal mode number
Perturbed electrostatic potential for given toroidal mode number
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/real(:,:) ⇹VFLT_2D¶Real part
Real part
1 |
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2 |
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/imaginary(:,:) ⇹VFLT_2D¶Imaginary part
Imaginary part
1 |
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2 |
time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/coefficients_real(:,:,:) ⇹VFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/phi_potential_perturbed/coefficients_imaginary(:,:,:) ⇹VFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbedVstructure¶Perturbed electromagnetic super-potential for given toroidal […]
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
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/real(:,:) ⇹VFLT_2D¶Real part
Real part
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2 |
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/imaginary(:,:) ⇹VFLT_2D¶Imaginary part
Imaginary part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/coefficients_real(:,:,:) ⇹VFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
1 |
|
2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/psi_potential_perturbed/coefficients_imaginary(:,:,:) ⇹VFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)AoS¶Local shear Alfven spectrum as a function of radius (only in […]
Local shear Alfven spectrum as a function of radius (only in case grid/dim1 is a radial coordinate)
1 |
time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/real(:) ⇹s^-1FLT_1D¶Real part of the frequency, for a given radial position and every […]
Real part of the frequency, for a given radial position and every root found at this position
1 |
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time_slice(itime)/toroidal_mode(i1)/plasma/alfven_frequency_spectrum(i2)/imaginary(:) ⇹s^-1FLT_1D¶Imaginary part of the frequency, for a given radial position […]
Imaginary part of the frequency, for a given radial position and every root found at this position
1 |
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time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwellstructure¶Maxwell stress tensor
Maxwell stress tensor
time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwell/real(:,:,:) ⇹N.m^-2FLT_3D¶Real part of the stress tensor, for various radial positions
Real part of the stress tensor, for various radial positions
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/stress_maxwell/imaginary(:,:,:) ⇹N.m^-2FLT_3D¶Imaginary part of the stress tensor, for various radial positions
Imaginary part of the stress tensor, for various radial positions
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynoldsstructure¶Reynolds stress tensor
Reynolds stress tensor
time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynolds/real(:,:,:) ⇹N.m^-2FLT_3D¶Real part of the stress tensor, for various radial positions
Real part of the stress tensor, for various radial positions
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/stress_reynolds/imaginary(:,:,:) ⇹N.m^-2FLT_3D¶Imaginary part of the stress tensor, for various radial positions
Imaginary part of the stress tensor, for various radial positions
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/ntvstructure¶Neoclassical toroidal viscosity tensor
Neoclassical toroidal viscosity tensor
time_slice(itime)/toroidal_mode(i1)/plasma/ntv/real(:,:,:) ⇹N.m^-2FLT_3D¶Real part of the stress tensor, for various radial positions
Real part of the stress tensor, for various radial positions
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/plasma/ntv/imaginary(:,:,:) ⇹N.m^-2FLT_3D¶Imaginary part of the stress tensor, for various radial positions
Imaginary part of the stress tensor, for various radial positions
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/vacuumstructure¶MHD modes in the vacuum
MHD modes in the vacuum
time_slice(itime)/toroidal_mode(i1)/vacuum/grid_typestructure¶Selection of one of a set of grid types
Selection of one of a set of grid types
This is an identifier. See poloidal_plane_coordinates_identifier for the available options.
time_slice(itime)/toroidal_mode(i1)/vacuum/grid_type/nameSTR_0D¶Short string identifier
Short string identifier
time_slice(itime)/toroidal_mode(i1)/vacuum/gridstructure¶Definition of the 2D grid (the content of dim1 and dim2 is defined […]
Definition of the 2D grid (the content of dim1 and dim2 is defined by the selected grid_type)
time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim1(:) ⇹mixedFLT_1D¶First dimension values
First dimension values
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time_slice(itime)/toroidal_mode(i1)/vacuum/grid/dim2(:) ⇹mixedFLT_1D¶Second dimension values
Second dimension values
1 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/grid/volume_element(:,:) ⇹m^3FLT_2D¶Elementary plasma volume of plasma enclosed in the cell formed […]
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)]
1 |
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2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_systemstructure¶Flux surface coordinate system of the equilibrium used for the […]
Flux surface coordinate system of the equilibrium used for the MHD calculation on a square grid of flux and poloidal angle
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid_typestructure¶Selection of one of a set of grid types
Selection of one of a set of grid types
This is an identifier. See poloidal_plane_coordinates_identifier for the available options.
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid_type/nameSTR_0D¶Short string identifier
Short string identifier
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/gridstructure¶Definition of the 2D grid
Definition of the 2D grid
time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim1(:) ⇹mixedFLT_1D¶First dimension values
First dimension values
1 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/dim2(:) ⇹mixedFLT_1D¶Second dimension values
Second dimension values
1 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/grid/volume_element(:,:) ⇹m^3FLT_2D¶Elementary plasma volume of plasma enclosed in the cell formed […]
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)]
1 |
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2 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/r(:,:) ⇹mFLT_2D¶Values of the major radius on the grid
Values of the major radius on the grid
1 |
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2 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/z(:,:) ⇹mFLT_2D¶Values of the Height on the grid
Values of the Height on the grid
1 |
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2 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/jacobian(:,:) ⇹mixedFLT_2D¶Absolute value of the jacobian of the coordinate system
Absolute value of the jacobian of the coordinate system
1 |
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2 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/tensor_covariant(:,:,:,:) ⇹mixedFLT_4D¶Covariant metric tensor on every point of the grid described […]
Covariant metric tensor on every point of the grid described by grid_type
1 |
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2 |
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3 |
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4 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/coordinate_system/tensor_contravariant(:,:,:,:) ⇹mixedFLT_4D¶Contravariant metric tensor on every point of the grid described […]
Contravariant metric tensor on every point of the grid described by grid_type
1 |
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2 |
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3 |
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4 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbedT.mstructure¶Pertubed vector potential for given toroidal mode number
Pertubed vector potential for given toroidal mode number
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1T.mstructure¶First coordinate (radial)
First coordinate (radial)
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/real(:,:) ⇹T.mFLT_2D¶Real part
Real part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/imaginary(:,:) ⇹T.mFLT_2D¶Imaginary part
Imaginary part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/coefficients_real(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
1 |
|
2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate1/coefficients_imaginary(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
1 |
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2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2T.mstructure¶Second coordinate (poloidal)
Second coordinate (poloidal)
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/real(:,:) ⇹T.mFLT_2D¶Real part
Real part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/imaginary(:,:) ⇹T.mFLT_2D¶Imaginary part
Imaginary part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/coefficients_real(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
1 |
|
2 |
|
3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate2/coefficients_imaginary(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
1 |
|
2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3T.mstructure¶Third coordinate (toroidal)
Third coordinate (toroidal)
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/real(:,:) ⇹T.mFLT_2D¶Real part
Real part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/imaginary(:,:) ⇹T.mFLT_2D¶Imaginary part
Imaginary part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/coefficients_real(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
1 |
|
2 |
|
3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/a_field_perturbed/coordinate3/coefficients_imaginary(:,:,:) ⇹T.mFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
1 |
|
2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbedTstructure¶Pertubed magnetic field for given toroidal mode number
Pertubed magnetic field for given toroidal mode number
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1Tstructure¶First coordinate (radial)
First coordinate (radial)
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/real(:,:) ⇹TFLT_2D¶Real part
Real part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/imaginary(:,:) ⇹TFLT_2D¶Imaginary part
Imaginary part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/coefficients_real(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
1 |
|
2 |
|
3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate1/coefficients_imaginary(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
1 |
|
2 |
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3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2Tstructure¶Second coordinate (poloidal)
Second coordinate (poloidal)
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/real(:,:) ⇹TFLT_2D¶Real part
Real part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/imaginary(:,:) ⇹TFLT_2D¶Imaginary part
Imaginary part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/coefficients_real(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
1 |
|
2 |
|
3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate2/coefficients_imaginary(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
1 |
|
2 |
|
3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3Tstructure¶Third coordinate (toroidal)
Third coordinate (toroidal)
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/real(:,:) ⇹TFLT_2D¶Real part
Real part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/imaginary(:,:) ⇹TFLT_2D¶Imaginary part
Imaginary part
1 |
|
2 |
time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/coefficients_real(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (real part) with finite elements, provided on the 2D grid
1 |
|
2 |
|
3 |
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time_slice(itime)/toroidal_mode(i1)/vacuum/b_field_perturbed/coordinate3/coefficients_imaginary(:,:,:) ⇹TFLT_3D¶Interpolation coefficients, to be used for a high precision evaluation […]
Interpolation coefficients, to be used for a high precision evaluation of the physical quantity (imaginary part) with finite elements, provided on the 2D grid
1 |
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2 |
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3 |
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