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MFC
Exascale flow solver
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Per-cell noncharacteristic boundary condition primitives applied in the ghost cells. More...
Functions/Subroutines | |
| subroutine | s_ghost_cell_extrapolation (q_prim_vf, bc_dir, bc_loc, k, l, q_t_sf) |
| Fill ghost cells by copying the nearest boundary cell value along the specified direction. | |
| subroutine | s_symmetry (q_prim_vf, bc_dir, bc_loc, k, l, pb_in, mv_in, q_t_sf) |
| Apply reflective (symmetry) boundary conditions by mirroring primitive variables and flipping the normal velocity component. | |
| subroutine | s_periodic (q_prim_vf, bc_dir, bc_loc, k, l, pb_in, mv_in, q_t_sf) |
| Apply periodic boundary conditions by copying values from the opposite domain boundary. | |
| subroutine | s_axis (q_prim_vf, pb_in, mv_in, k, l) |
| Apply axis boundary conditions for cylindrical coordinates by reflecting values across the axis with azimuthal phase shift. | |
| subroutine | s_slip_wall (q_prim_vf, bc_dir, bc_loc, k, l, q_t_sf) |
| Apply slip wall boundary conditions by extrapolating scalars and reflecting the wall-normal velocity component. | |
| subroutine | s_no_slip_wall (q_prim_vf, bc_dir, bc_loc, k, l, q_t_sf) |
| Apply no-slip wall boundary conditions by reflecting and negating all velocity components at the wall. | |
| subroutine | s_dirichlet (q_prim_vf, bc_dir, bc_loc, k, l, q_t_sf) |
| Apply Dirichlet boundary conditions by prescribing ghost cell values from stored boundary buffers. | |
| subroutine | s_qbmm_extrapolation (bc_dir, bc_loc, k, l, pb_in, mv_in) |
| Extrapolate QBMM bubble pressure and mass-vapor variables into ghost cells by copying boundary values. | |
| subroutine | s_color_function_periodic (c_divs, bc_dir, bc_loc, k, l) |
| Apply periodic boundary conditions to the color function and its divergence fields. | |
| subroutine | s_color_function_reflective (c_divs, bc_dir, bc_loc, k, l) |
| Apply reflective boundary conditions to the color function and its divergence fields. | |
| subroutine | s_color_function_ghost_cell_extrapolation (c_divs, bc_dir, bc_loc, k, l) |
| Extrapolate the color function and its divergence into ghost cells by copying boundary values. | |
| subroutine | s_f_igr_periodic (jac_sf, bc_dir, bc_loc, k, l) |
| Apply periodic boundary conditions to the IGR Jacobian field by copying values from the opposite domain boundary. | |
| subroutine | s_f_igr_reflective (jac_sf, bc_dir, bc_loc, k, l) |
| Apply reflective boundary conditions to the IGR Jacobian field by mirroring values across the boundary. | |
| subroutine | s_f_igr_ghost_cell_extrapolation (jac_sf, bc_dir, bc_loc, k, l) |
| Extrapolate the IGR Jacobian field into ghost cells by copying boundary values. | |
| subroutine | s_beta_periodic (q_beta, kahan_comp, bc_dir, bc_loc, k, l, nvar) |
| subroutine | s_beta_extrapolation (q_beta, bc_dir, bc_loc, k, l, nvar) |
| subroutine | s_beta_reflective (q_beta, kahan_comp, bc_dir, bc_loc, k, l, nvar) |
| subroutine | s_grid_periodic_bc (bc_dir, bc_loc, offset_dir) |
| Apply periodic boundary conditions to grid variables by copying cell widths from opposite domain boundary. | |
| subroutine | s_grid_reflective_bc (bc_dir, bc_loc, offset_dir) |
| Apply reflective boundary conditions to grid variables by mirroring cell widths across the boundary. | |
| subroutine | s_grid_ghost_cell_extrapolation_bc (bc_dir, bc_loc, offset_dir) |
| Extrapolate grid variables by copying boundary cell width into ghost cells. | |
| subroutine | s_grid_axis_bc (bc_loc, offset_dir) |
| Apply axis boundary conditions to grid variables for cylindrical coordinates. | |
Variables | |
| type(scalar_field), dimension(:,:), allocatable | bc_buffers |
Per-cell noncharacteristic boundary condition primitives applied in the ghost cells.
| subroutine m_boundary_primitives::s_axis | ( | type(scalar_field), dimension(sys_size), intent(inout) | q_prim_vf, |
| real(stp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:,1:), intent(inout), optional | pb_in, | ||
| real(stp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:,1:), intent(inout), optional | mv_in, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l ) |
Apply axis boundary conditions for cylindrical coordinates by reflecting values across the axis with azimuthal phase shift.
Definition at line 915 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_beta_extrapolation | ( | type(scalar_field), dimension(num_dims + 1), intent(inout) | q_beta, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| integer, intent(in) | nvar ) |
Definition at line 2221 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_beta_periodic | ( | type(scalar_field), dimension(num_dims + 1), intent(inout) | q_beta, |
| type(scalar_field), dimension(num_dims + 1), intent(inout) | kahan_comp, | ||
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| integer, intent(in) | nvar ) |
Definition at line 2113 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_beta_reflective | ( | type(scalar_field), dimension(num_dims + 1), intent(inout) | q_beta, |
| type(scalar_field), dimension(num_dims + 1), intent(inout) | kahan_comp, | ||
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| integer, intent(in) | nvar ) |
Definition at line 2310 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_color_function_ghost_cell_extrapolation | ( | type(scalar_field), dimension(num_dims + 1), intent(inout) | c_divs, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l ) |
Extrapolate the color function and its divergence into ghost cells by copying boundary values.
Definition at line 1794 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_color_function_periodic | ( | type(scalar_field), dimension(num_dims + 1), intent(inout) | c_divs, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l ) |
Apply periodic boundary conditions to the color function and its divergence fields.
Definition at line 1592 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_color_function_reflective | ( | type(scalar_field), dimension(num_dims + 1), intent(inout) | c_divs, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l ) |
Apply reflective boundary conditions to the color function and its divergence fields.
Definition at line 1681 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_dirichlet | ( | type(scalar_field), dimension(sys_size), intent(inout) | q_prim_vf, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| type(scalar_field), intent(inout), optional | q_t_sf ) |
Apply Dirichlet boundary conditions by prescribing ghost cell values from stored boundary buffers.
| [in,out] | q_t_sf | x-direction |
| [in,out] | q_t_sf | bc_xend |
| [in,out] | q_t_sf | y-direction |
| [in,out] | q_t_sf | bc_ybeg |
| [in,out] | q_t_sf | bc_yend |
| [in,out] | q_t_sf | z-direction |
| [in,out] | q_t_sf | bc_zbeg |
| [in,out] | q_t_sf | bc_zend |
Definition at line 1377 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_f_igr_ghost_cell_extrapolation | ( | type(scalar_field), dimension(1:), intent(inout) | jac_sf, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l ) |
Extrapolate the IGR Jacobian field into ghost cells by copying boundary values.
Definition at line 2037 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_f_igr_periodic | ( | type(scalar_field), dimension(1:), intent(inout) | jac_sf, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l ) |
Apply periodic boundary conditions to the IGR Jacobian field by copying values from the opposite domain boundary.
Definition at line 1883 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_f_igr_reflective | ( | type(scalar_field), dimension(1:), intent(inout) | jac_sf, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l ) |
Apply reflective boundary conditions to the IGR Jacobian field by mirroring values across the boundary.
Definition at line 1960 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_ghost_cell_extrapolation | ( | type(scalar_field), dimension(sys_size), intent(inout) | q_prim_vf, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| type(scalar_field), intent(inout), optional | q_t_sf ) |
Fill ghost cells by copying the nearest boundary cell value along the specified direction.
| [in,out] | q_t_sf | x-direction |
| [in,out] | q_t_sf | bc_xend |
| [in,out] | q_t_sf | y-direction |
| [in,out] | q_t_sf | bc_ybeg |
| [in,out] | q_t_sf | bc_yend |
| [in,out] | q_t_sf | z-direction |
| [in,out] | q_t_sf | bc_zbeg |
| [in,out] | q_t_sf | bc_zend |
Definition at line 359 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_grid_axis_bc | ( | integer, intent(in) | bc_loc, |
| type(int_bounds_info), intent(in) | offset_dir ) |
Apply axis boundary conditions to grid variables for cylindrical coordinates.
Definition at line 2688 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_grid_ghost_cell_extrapolation_bc | ( | integer, intent(in) | bc_dir, |
| integer, intent(in) | bc_loc, | ||
| type(int_bounds_info), intent(in) | offset_dir ) |
Extrapolate grid variables by copying boundary cell width into ghost cells.
Definition at line 2611 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_grid_periodic_bc | ( | integer, intent(in) | bc_dir, |
| integer, intent(in) | bc_loc, | ||
| type(int_bounds_info), intent(in) | offset_dir ) |
Apply periodic boundary conditions to grid variables by copying cell widths from opposite domain boundary.
Definition at line 2457 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_grid_reflective_bc | ( | integer, intent(in) | bc_dir, |
| integer, intent(in) | bc_loc, | ||
| type(int_bounds_info), intent(in) | offset_dir ) |
Apply reflective boundary conditions to grid variables by mirroring cell widths across the boundary.
Definition at line 2534 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_no_slip_wall | ( | type(scalar_field), dimension(sys_size), intent(inout) | q_prim_vf, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| type(scalar_field), intent(inout), optional | q_t_sf ) |
Apply no-slip wall boundary conditions by reflecting and negating all velocity components at the wall.
| [in,out] | q_t_sf | x-direction |
| [in,out] | q_t_sf | bc_xbeg |
| [in,out] | q_t_sf | bc_xend |
| [in,out] | q_t_sf | y-direction |
| [in,out] | q_t_sf | bc_ybeg |
| [in,out] | q_t_sf | bc_yend |
| [in,out] | q_t_sf | z-direction |
| [in,out] | q_t_sf | bc_zbeg |
| [in,out] | q_t_sf | bc_zend |
Definition at line 1170 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_periodic | ( | type(scalar_field), dimension(sys_size), intent(inout) | q_prim_vf, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| real(stp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:,1:), intent(inout), optional | pb_in, | ||
| real(stp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:,1:), intent(inout), optional | mv_in, | ||
| type(scalar_field), intent(inout), optional | q_t_sf ) |
Apply periodic boundary conditions by copying values from the opposite domain boundary.
| [in,out] | q_t_sf | x-direction |
| [in,out] | q_t_sf | bc_xbeg |
| [in,out] | q_t_sf | bc_xend |
| [in,out] | q_t_sf | y-direction |
| [in,out] | q_t_sf | bc_ybeg |
| [in,out] | q_t_sf | bc_yend |
| [in,out] | q_t_sf | z-direction |
| [in,out] | q_t_sf | bc_zbeg |
| [in,out] | q_t_sf | bc_zend |
Definition at line 742 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_qbmm_extrapolation | ( | integer, intent(in) | bc_dir, |
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| real(stp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:,1:), intent(inout), optional | pb_in, | ||
| real(stp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:,1:), intent(inout), optional | mv_in ) |
Extrapolate QBMM bubble pressure and mass-vapor variables into ghost cells by copying boundary values.
Definition at line 1505 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_slip_wall | ( | type(scalar_field), dimension(sys_size), intent(inout) | q_prim_vf, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| type(scalar_field), intent(inout), optional | q_t_sf ) |
Apply slip wall boundary conditions by extrapolating scalars and reflecting the wall-normal velocity component.
| [in,out] | q_t_sf | x-direction |
| [in,out] | q_t_sf | bc_xbeg |
| [in,out] | q_t_sf | bc_xend |
| [in,out] | q_t_sf | y-direction |
| [in,out] | q_t_sf | bc_ybeg |
| [in,out] | q_t_sf | bc_yend |
| [in,out] | q_t_sf | z-direction |
| [in,out] | q_t_sf | bc_zbeg |
| [in,out] | q_t_sf | bc_zend |
Definition at line 984 of file m_boundary_primitives.fpp.f90.
| subroutine m_boundary_primitives::s_symmetry | ( | type(scalar_field), dimension(sys_size), intent(inout) | q_prim_vf, |
| integer, intent(in) | bc_dir, | ||
| integer, intent(in) | bc_loc, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| real(stp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:,1:), intent(inout), optional | pb_in, | ||
| real(stp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:,1:), intent(inout), optional | mv_in, | ||
| type(scalar_field), intent(inout), optional | q_t_sf ) |
Apply reflective (symmetry) boundary conditions by mirroring primitive variables and flipping the normal velocity component.
| [in,out] | q_t_sf | x-direction |
| [in,out] | q_t_sf | bc_xbeg |
| [in,out] | q_t_sf | bc_xend |
| [in,out] | q_t_sf | y-direction |
| [in,out] | q_t_sf | bc_ybeg |
| [in,out] | q_t_sf | bc_yend |
| [in,out] | q_t_sf | z-direction |
| [in,out] | q_t_sf | bc_zbeg |
| [in,out] | q_t_sf | bc_zend |
Definition at line 480 of file m_boundary_primitives.fpp.f90.
| type(scalar_field), dimension(:,:), allocatable m_boundary_primitives::bc_buffers |
Definition at line 343 of file m_boundary_primitives.fpp.f90.