|
MFC
Exascale flow solver
|
Contains module m_rhs. More...
Go to the source code of this file.
Modules | |
| module | m_rhs |
| Assembles the right-hand side of the governing equations using finite-volume flux differencing, Riemann solvers, and physical source terms. | |
Functions/Subroutines | |
| impure subroutine, public | m_rhs::s_initialize_rhs_module |
| The computation of parameters, the allocation of memory, the association of pointers and/or the execution of any other procedures that are necessary to setup the module. | |
| impure subroutine, public | m_rhs::s_compute_rhs (q_cons_vf, q_t_sf, q_prim_vf, bc_type, rhs_vf, pb_in, rhs_pb, mv_in, rhs_mv, t_step, time_avg, stage) |
| Computes the right-hand side of the semi-discrete governing equations for a single time stage. | |
| subroutine | m_rhs::s_compute_advection_source_term (idir, rhs_vf, q_cons_vf, q_prim_vf, flux_src_n_vf) |
| Accumulates advection source contributions from a given coordinate direction into the RHS. | |
| subroutine | s_add_directional_advection_source_terms (current_idir, rhs_vf_arg, q_cons_vf_arg, q_prim_vf_arg, flux_src_n_vf_arg, kterm_arg) |
| Adds the advection source flux-difference terms for a single coordinate direction to the RHS. | |
| subroutine | m_rhs::s_compute_additional_physics_rhs (idir, q_prim_vf, rhs_vf, flux_src_n_in, dq_prim_dx_vf, dq_prim_dy_vf, dq_prim_dz_vf) |
| Adds viscous, surface-tension, and species-diffusion source flux contributions to the RHS for a given direction. | |
| subroutine | m_rhs::s_reconstruct_cell_boundary_values (v_vf, vl_x, vl_y, vl_z, vr_x, vr_y, vr_z, norm_dir) |
| The purpose of this subroutine is to WENO-reconstruct the left and the right cell-boundary values, including values at the Gaussian quadrature points, from the cell-averaged variables. | |
| subroutine | m_rhs::s_reconstruct_cell_boundary_values_first_order (v_vf, vl_x, vl_y, vl_z, vr_x, vr_y, vr_z, norm_dir) |
| Performs first-order (piecewise constant) reconstruction of left and right cell-boundary values. | |
| impure subroutine, public | m_rhs::s_finalize_rhs_module |
| Module deallocation and/or disassociation procedures. | |
Variables | |
| type(vector_field) | m_rhs::q_cons_qp |
| type(vector_field) | m_rhs::q_prim_qp |
| type(scalar_field), dimension(:), allocatable | m_rhs::tau_re_vf |
| type(vector_field) | m_rhs::gm_alpha_qp |
| The gradient magnitude of the volume fractions at cell-interior Gaussian quadrature points. gm_alpha_qp is calculated from individual first-order spatial derivatives located in dq_prim_ds_qp. | |
| type(vector_field), dimension(:), allocatable | m_rhs::ql_prim |
| type(vector_field), dimension(:), allocatable | m_rhs::qr_prim |
| type(int_bounds_info) | m_rhs::iv |
| Vector field indical bounds. | |
| real(wp), dimension(:, :, :), allocatable | m_rhs::blkmod1 |
| real(wp), dimension(:, :, :), allocatable | m_rhs::blkmod2 |
| real(wp), dimension(:, :, :), allocatable | m_rhs::alpha1 |
| real(wp), dimension(:, :, :), allocatable | m_rhs::alpha2 |
| real(wp), dimension(:, :, :), allocatable | m_rhs::kterm |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::ql_rsx_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::ql_rsy_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::ql_rsz_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::qr_rsx_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::qr_rsy_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::qr_rsz_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::dql_rsx_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::dql_rsy_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::dql_rsz_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::dqr_rsx_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::dqr_rsy_vf |
| real(wp), dimension(:, :, :, :), allocatable | m_rhs::dqr_rsz_vf |
| real(wp), dimension(:, :, :), allocatable | m_rhs::nbub |
| Bubble number density. | |
The first-order spatial derivatives of the primitive variables at cell- | |
interior Gaussian quadrature points. These are WENO-reconstructed from their respective cell-average values, obtained through the application of the divergence theorem on the integral-average cell-boundary values of the primitive variables, located in qK_prim_n, where K = L or R. | |
| type(vector_field), dimension(:), allocatable | m_rhs::dq_prim_dx_qp |
| type(vector_field), dimension(:), allocatable | m_rhs::dq_prim_dy_qp |
| type(vector_field), dimension(:), allocatable | m_rhs::dq_prim_dz_qp |
The left and right WENO-reconstructed cell-boundary values of the cell- | |
average gradient magnitude of volume fractions, located in gm_alpha_qp. | |
| type(vector_field), dimension(:), allocatable | m_rhs::dql_prim_dx_n |
| type(vector_field), dimension(:), allocatable | m_rhs::dql_prim_dy_n |
| type(vector_field), dimension(:), allocatable | m_rhs::dql_prim_dz_n |
| type(vector_field), dimension(:), allocatable | m_rhs::dqr_prim_dx_n |
| type(vector_field), dimension(:), allocatable | m_rhs::dqr_prim_dy_n |
| type(vector_field), dimension(:), allocatable | m_rhs::dqr_prim_dz_n |
| type(vector_field), dimension(:), allocatable | m_rhs::gm_alphal_n |
| type(vector_field), dimension(:), allocatable | m_rhs::gm_alphar_n |
The cell-boundary values of the fluxes (src - source, gsrc - geometrical | |
source). These are computed by applying the chosen Riemann problem solver .on the left and right cell-boundary values of the primitive variables | |
| type(vector_field), dimension(:), allocatable | m_rhs::flux_n |
| type(vector_field), dimension(:), allocatable | m_rhs::flux_src_n |
| type(vector_field), dimension(:), allocatable | m_rhs::flux_gsrc_n |
Indical bounds in the x-, y- and z-directions | |
| type(int_bounds_info) | m_rhs::irx |
| type(int_bounds_info) | m_rhs::iry |
| type(int_bounds_info) | m_rhs::irz |
| type(int_bounds_info) | m_rhs::is1 |
| type(int_bounds_info) | m_rhs::is2 |
| type(int_bounds_info) | m_rhs::is3 |
Saved fluxes for testing | |
| type(scalar_field) | m_rhs::alf_sum |
Contains module m_rhs.
Definition in file m_rhs.fpp.f90.
|
private |
Adds the advection source flux-difference terms for a single coordinate direction to the RHS.
Definition at line 8013 of file m_rhs.fpp.f90.