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MFC
Exascale flow solver
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MFC
Exascale flow solver
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HLLC Riemann solver with contact restoration, Toro et al. Shock Waves (1994). More...
Functions/Subroutines | |
| subroutine | s_hllc_riemann_solver (ql_prim_rsx_vf, dql_prim_dx_vf, dql_prim_dy_vf, dql_prim_dz_vf, ql_prim_vf, qr_prim_rsx_vf, dqr_prim_dx_vf, dqr_prim_dy_vf, dqr_prim_dz_vf, qr_prim_vf, q_prim_vf, flux_vf, flux_src_vf, flux_gsrc_vf, norm_dir, ix, iy, iz) |
| HLLC Riemann solver with contact restoration, Toro et al. Shock Waves (1994). | |
HLLC Riemann solver with contact restoration, Toro et al. Shock Waves (1994).
| subroutine m_riemann_solver_hllc::s_hllc_riemann_solver | ( | real(wp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:), intent(inout) | ql_prim_rsx_vf, |
| type(scalar_field), dimension(:), intent(inout), allocatable | dql_prim_dx_vf, | ||
| type(scalar_field), dimension(:), intent(inout), allocatable | dql_prim_dy_vf, | ||
| type(scalar_field), dimension(:), intent(inout), allocatable | dql_prim_dz_vf, | ||
| type(scalar_field), dimension(:), intent(inout), allocatable | ql_prim_vf, | ||
| real(wp), dimension(idwbuff(1)%beg:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:), intent(inout) | qr_prim_rsx_vf, | ||
| type(scalar_field), dimension(:), intent(inout), allocatable | dqr_prim_dx_vf, | ||
| type(scalar_field), dimension(:), intent(inout), allocatable | dqr_prim_dy_vf, | ||
| type(scalar_field), dimension(:), intent(inout), allocatable | dqr_prim_dz_vf, | ||
| type(scalar_field), dimension(:), intent(inout), allocatable | qr_prim_vf, | ||
| type(scalar_field), dimension(sys_size), intent(in) | q_prim_vf, | ||
| type(scalar_field), dimension(sys_size), intent(inout) | flux_vf, | ||
| type(scalar_field), dimension(sys_size), intent(inout) | flux_src_vf, | ||
| type(scalar_field), dimension(sys_size), intent(inout) | flux_gsrc_vf, | ||
| integer, intent(in) | norm_dir, | ||
| type(int_bounds_info), intent(in) | ix, | ||
| type(int_bounds_info), intent(in) | iy, | ||
| type(int_bounds_info), intent(in) | iz ) |
HLLC Riemann solver with contact restoration, Toro et al. Shock Waves (1994).
The computation of c_avg does not require all the variables, and therefore the non '_avg'
The computation of c_avg does not require all the variables, and therefore the non '_avg'
The computation of c_avg does not require all the variables, and therefore the non '_avg'
gamma_method = 1: Ref. Section 2.3.1 Formulation of doi:10.7907/ZKW8-ES97.
gamma_method = 2: c_p / c_v where c_p, c_v are specific heats.
The computation of c_avg does not require all the variables, and therefore the non '_avg'
The computation of c_avg does not require all the variables, and therefore the non '_avg'
The computation of c_avg does not require all the variables, and therefore the non '_avg'
The computation of c_avg does not require all the variables, and therefore the non '_avg'
gamma_method = 1: Ref. Section 2.3.1 Formulation of doi:10.7907/ZKW8-ES97.
gamma_method = 2: c_p / c_v where c_p, c_v are specific heats.
The computation of c_avg does not require all the variables, and therefore the non '_avg'
The computation of c_avg does not require all the variables, and therefore the non '_avg'
The computation of c_avg does not require all the variables, and therefore the non '_avg'
The computation of c_avg does not require all the variables, and therefore the non '_avg'
gamma_method = 1: Ref. Section 2.3.1 Formulation of doi:10.7907/ZKW8-ES97.
gamma_method = 2: c_p / c_v where c_p, c_v are specific heats.
The computation of c_avg does not require all the variables, and therefore the non '_avg'
Definition at line 358 of file m_riemann_solver_hllc.fpp.f90.