Computation of ion stress function G = G_flow + G_heat with "beyond Braginskii extensions" according to parameters
| Type | Intent | Optional | Attributes | Name | ||
|---|---|---|---|---|---|---|
| class(gyroviscosity_t), | intent(in) | :: | self |
Instance of type |
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| type(mesh_cart_t), | intent(in) | :: | mesh_cano |
Mesh (canonical) within poloidal plane |
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| class(equilibrium_storage_t), | intent(in) | :: | equi_on_cano |
Equilibrim quantities on canonical mesh |
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| type(inplane_operators_t), | intent(in) | :: | opsinplane_cano |
In-plane operators (canonical) |
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| type(parallel_map_t), | intent(in) | :: | map |
Parallel map |
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| real(kind=GP), | intent(in), | dimension(mesh_cano%get_n_points()) | :: | ne_v |
Electron density |
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| real(kind=GP), | intent(in), | dimension(mesh_cano%get_n_points()) | :: | pot_v |
Electrostatic potential |
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| real(kind=GP), | intent(in), | dimension(mesh_cano%get_n_points()) | :: | ti_v |
Ion temperature |
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| real(kind=GP), | intent(in), | dimension(mesh_cano%get_n_points()) | :: | apar_fluct_cano_v |
Fluctuation of apar used for flutter operators It is assumed that communication has already been done to do mapping to canonical mesh |
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| real(kind=GP), | intent(out), | dimension(mesh_cano%get_n_points()) | :: | gstress |
Values of ion viscous stress function G |
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| logical, | intent(in), | optional | :: | eval_flow_crv |
If true computes part of G_flow arising from curvature terms (default = T) This feature is useful for technical reasons, when only evaluation of individual parts of G is needed |
|
| logical, | intent(in), | optional | :: | eval_flow_par |
If true computes computes part of G_flow arising from parallel divergence of upar (default = T) |
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| logical, | intent(in), | optional | :: | eval_heat_crv |
If true computes part of G_heat arising from curvature terms (default = T) |
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| logical, | intent(in), | optional | :: | eval_heat_par |
If true computes part of G_flow arising from paralle divergence of qipar (default = T) |