Semi-Lagrangian Library
Modular library for kinetic and gyrokinetic simulations of plasmas in fusion energy devices.
|
Maxwell solver class with pseudospectral method. More...
Private Member Functions | |
procedure | compute_e_b => sll_s_compute_e_b_1d |
procedure | compute_e_from_b => compute_field_from_field_1d_ps |
procedure | compute_b_from_e => compute_field_from_field_1d_ps |
procedure | compute_curl_part => compute_curl_part_1d_ps |
procedure | compute_e_from_rho => compute_e_from_rho_1d_ps |
procedure | compute_rho_from_e => compute_rho_from_e_1d_ps |
procedure | compute_e_from_j => compute_e_from_j_1d_ps |
procedure | compute_rhs_from_function |
procedure | l2norm_squared => l2norm_squared_1d_ps |
procedure | inner_product => inner_product_1d_ps |
procedure | l2projection |
procedure | transform_dofs => transform_dofs_1d_ps |
procedure | multiply_mass => multiply_mass_1d_ps |
procedure | invert_mass => invert_mass_1d_ps |
procedure | multiply_g |
procedure | multiply_gt |
procedure | free => free_1d_ps |
procedure | init => init_1d_ps |
procedure | grad_proj0 |
procedure | proj1_grad |
procedure | compute_phi_from_rho => compute_phi_from_rho_1d_ps |
procedure | compute_phi_from_j => compute_phi_from_j_1d_ps |
Private Attributes | |
type(sll_t_fft) | plan_fw |
fft plan (forward) More... | |
type(sll_t_fft) | plan_bw |
fft plan (backward) More... | |
logical | strong_ampere = .false. |
flag to switch between strong and weak Ampere formulation More... | |
Maxwell solver class with pseudospectral method.
Definition at line 39 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 68 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 70 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 64 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 66 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 76 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 72 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 99 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 98 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 74 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 78 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 91 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 95 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 92 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 82 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 88 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 80 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 84 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 89 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 90 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 87 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 96 of file sll_m_maxwell_1d_ps.F90.
|
private |
Definition at line 86 of file sll_m_maxwell_1d_ps.F90.
|
private |
fft plan (backward)
Definition at line 43 of file sll_m_maxwell_1d_ps.F90.
|
private |
fft plan (forward)
Definition at line 42 of file sll_m_maxwell_1d_ps.F90.
|
privateinherited |
flag to switch between strong and weak Ampere formulation
tolerance for the field solver
Definition at line 35 of file sll_m_maxwell_1d_base.F90.