Shared Riemann-solver module state and the per-sweep setup, state-buffer population, viscous source flux, and finalization helpers. More...

Functions/Subroutines
subroutine	s_compute_viscous_source_flux (vell_vf, dvell_dx_vf, dvell_dy_vf, dvell_dz_vf, velr_vf, dvelr_dx_vf, dvelr_dy_vf, dvelr_dz_vf, flux_src_vf, q_prim_vf, norm_dir, ix, iy, iz)
	Dispatch to the subroutines that are utilized to compute the viscous source fluxes for either Cartesian or cylindrical geometries. For more information please refer to: 1) s_compute_cartesian_viscous_source_flux 2) s_compute_cylindrical_viscous_source_flux.
subroutine	s_populate_riemann_states_variables_buffers (ql_prim_rsx_vf, dql_prim_dx_vf, dql_prim_dy_vf, dql_prim_dz_vf, qr_prim_rsx_vf, dqr_prim_dx_vf, dqr_prim_dy_vf, dqr_prim_dz_vf, norm_dir, ix, iy, iz)
	Populate the left and right Riemann state variable buffers based on boundary conditions.
subroutine	s_initialize_riemann_solver (flux_src_vf, norm_dir)
	Set up the chosen Riemann solver algorithm for the current direction.
subroutine	s_compute_cylindrical_viscous_source_flux (vell_vf, dvell_dx_vf, dvell_dy_vf, dvell_dz_vf, velr_vf, dvelr_dx_vf, dvelr_dy_vf, dvelr_dz_vf, flux_src_vf, q_prim_vf, norm_dir, ix, iy, iz)
	Compute cylindrical viscous source flux contributions for momentum and energy.
subroutine	s_compute_cartesian_viscous_source_flux (dvell_dx_vf, dvell_dy_vf, dvell_dz_vf, dvelr_dx_vf, dvelr_dy_vf, dvelr_dz_vf, flux_src_vf, q_prim_vf, norm_dir)
	Compute Cartesian viscous source flux contributions for momentum and energy.
subroutine	s_calculate_shear_stress_tensor (vel_grad_avg, re_shear, divergence_v, tau_shear_out)
	Compute shear stress tensor components.
subroutine	s_calculate_bulk_stress_tensor (re_bulk, divergence_v, tau_bulk_out)
	Compute bulk stress tensor components (diagonal only).
subroutine	s_finalize_riemann_solver (flux_vf, flux_src_vf, flux_gsrc_vf, norm_dir)
	Deallocation and/or disassociation procedures that are needed to finalize the selected Riemann problem solver.

Variables
real(wp), dimension(:,:,:,:), allocatable	vel_src_rsx_vf
real(wp), dimension(:,:,:,:), allocatable	mom_sp_rsx_vf
real(wp), dimension(:,:,:,:), allocatable	re_avg_rsx_vf
real(wp), dimension(:), allocatable	gs_rs
real(wp), dimension(:,:), allocatable	res_gs

real(wp), dimension(:,:,:,:), allocatable	flux_rsx_vf
	The cell-boundary values of the fluxes (src - source) that are computed through the chosen Riemann problem solver, and the direct evaluation of source terms, by using the left and right states given in qK_prim_rs_vf, dqK_prim_ds_vf where ds = dx, dy or dz.
real(wp), dimension(:,:,:,:), allocatable	flux_src_rsx_vf

real(wp), dimension(:,:,:,:), allocatable	flux_gsrc_rsx_vf
	The cell-boundary values of the geometrical source flux that are computed through the chosen Riemann problem solver by using the left and right states given in qK_prim_rs_vf. Currently 2D axisymmetric for inviscid only.
Indical bounds in the s1-, s2- and s3-directions
type(int_bounds_info)	is1
type(int_bounds_info)	is2
type(int_bounds_info)	is3
type(int_bounds_info)	isx
type(int_bounds_info)	isy
type(int_bounds_info)	isz

Detailed Description

Shared Riemann-solver module state and the per-sweep setup, state-buffer population, viscous source flux, and finalization helpers.

Function/Subroutine Documentation

◆ s_calculate_bulk_stress_tensor()

subroutine m_riemann_state::s_calculate_bulk_stress_tensor	(	real(wp), intent(in)	re_bulk,
		real(wp), intent(in)	divergence_v,
		real(wp), dimension(num_dims, num_dims), intent(out)	tau_bulk_out )

Compute bulk stress tensor components (diagonal only).

Definition at line 2490 of file m_riemann_state.fpp.f90.

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◆ s_calculate_shear_stress_tensor()

subroutine m_riemann_state::s_calculate_shear_stress_tensor	(	real(wp), dimension(num_dims, num_dims), intent(in)	vel_grad_avg,
		real(wp), intent(in)	re_shear,
		real(wp), intent(in)	divergence_v,
		real(wp), dimension(num_dims, num_dims), intent(out)	tau_shear_out )

Compute shear stress tensor components.

Definition at line 2447 of file m_riemann_state.fpp.f90.

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◆ s_compute_cartesian_viscous_source_flux()

subroutine m_riemann_state::s_compute_cartesian_viscous_source_flux	(	type(scalar_field), dimension(num_dims), intent(in)	dvell_dx_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvell_dy_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvell_dz_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvelr_dx_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvelr_dy_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvelr_dz_vf,
		type(scalar_field), dimension(sys_size), intent(inout)	flux_src_vf,
		type(scalar_field), dimension(sys_size), intent(in)	q_prim_vf,
		integer, intent(in)	norm_dir )

Compute Cartesian viscous source flux contributions for momentum and energy.

Definition at line 2249 of file m_riemann_state.fpp.f90.

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◆ s_compute_cylindrical_viscous_source_flux()

subroutine m_riemann_state::s_compute_cylindrical_viscous_source_flux	(	type(scalar_field), dimension(num_dims), intent(in)	vell_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvell_dx_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvell_dy_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvell_dz_vf,
		type(scalar_field), dimension(num_dims), intent(in)	velr_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvelr_dx_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvelr_dy_vf,
		type(scalar_field), dimension(num_dims), intent(in)	dvelr_dz_vf,
		type(scalar_field), dimension(sys_size), intent(inout)	flux_src_vf,
		type(scalar_field), dimension(sys_size), intent(in)	q_prim_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 )

Compute cylindrical viscous source flux contributions for momentum and energy.

Interface velocity ( \(v_1,v_2,v_3\)) (grid directions) for viscous work.

Shear stress vector ( \(\sigma_{N1}, \sigma_{N2}, \sigma_{N3}\)) on N-face (grid directions).

Definition at line 1986 of file m_riemann_state.fpp.f90.

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◆ s_compute_viscous_source_flux()

subroutine m_riemann_state::s_compute_viscous_source_flux	(	type(scalar_field), dimension(num_vels), intent(in)	vell_vf,
		type(scalar_field), dimension(num_vels), intent(in)	dvell_dx_vf,
		type(scalar_field), dimension(num_vels), intent(in)	dvell_dy_vf,
		type(scalar_field), dimension(num_vels), intent(in)	dvell_dz_vf,
		type(scalar_field), dimension(num_vels), intent(in)	velr_vf,
		type(scalar_field), dimension(num_vels), intent(in)	dvelr_dx_vf,
		type(scalar_field), dimension(num_vels), intent(in)	dvelr_dy_vf,
		type(scalar_field), dimension(num_vels), intent(in)	dvelr_dz_vf,
		type(scalar_field), dimension(sys_size), intent(inout)	flux_src_vf,
		type(scalar_field), dimension(sys_size), intent(in)	q_prim_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 )

Dispatch to the subroutines that are utilized to compute the viscous source fluxes for either Cartesian or cylindrical geometries. For more information please refer to: 1) s_compute_cartesian_viscous_source_flux 2) s_compute_cylindrical_viscous_source_flux.

Definition at line 463 of file m_riemann_state.fpp.f90.

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◆ s_finalize_riemann_solver()

subroutine m_riemann_state::s_finalize_riemann_solver	(	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 )

Deallocation and/or disassociation procedures that are needed to finalize the selected Riemann problem solver.

Definition at line 2526 of file m_riemann_state.fpp.f90.

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◆ s_initialize_riemann_solver()

subroutine m_riemann_state::s_initialize_riemann_solver	(	type(scalar_field), dimension(sys_size), intent(inout)	flux_src_vf,
		integer, intent(in)	norm_dir )

Set up the chosen Riemann solver algorithm for the current direction.

Definition at line 1567 of file m_riemann_state.fpp.f90.

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◆ s_populate_riemann_states_variables_buffers()

subroutine m_riemann_state::s_populate_riemann_states_variables_buffers	(	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,
		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,
		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 )

Populate the left and right Riemann state variable buffers based on boundary conditions.

Definition at line 486 of file m_riemann_state.fpp.f90.

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Variable Documentation

◆ flux_gsrc_rsx_vf

real(wp), dimension(:,:,:,:), allocatable m_riemann_state::flux_gsrc_rsx_vf

The cell-boundary values of the geometrical source flux that are computed through the chosen Riemann problem solver by using the left and right states given in qK_prim_rs_vf. Currently 2D axisymmetric for inviscid only.

Definition at line 359 of file m_riemann_state.fpp.f90.

◆ flux_rsx_vf

real(wp), dimension(:,:,:,:), allocatable m_riemann_state::flux_rsx_vf

The cell-boundary values of the fluxes (src - source) that are computed through the chosen Riemann problem solver, and the direct evaluation of source terms, by using the left and right states given in qK_prim_rs_vf, dqK_prim_ds_vf where ds = dx, dy or dz.

Definition at line 342 of file m_riemann_state.fpp.f90.

◆ flux_src_rsx_vf

real(wp), dimension(:,:,:,:), allocatable m_riemann_state::flux_src_rsx_vf

Definition at line 342 of file m_riemann_state.fpp.f90.

◆ gs_rs

real(wp), dimension(:), allocatable m_riemann_state::gs_rs

Definition at line 432 of file m_riemann_state.fpp.f90.

◆ is1

type(int_bounds_info) m_riemann_state::is1

Definition at line 416 of file m_riemann_state.fpp.f90.

◆ is2

type(int_bounds_info) m_riemann_state::is2

Definition at line 416 of file m_riemann_state.fpp.f90.

◆ is3

type(int_bounds_info) m_riemann_state::is3

Definition at line 416 of file m_riemann_state.fpp.f90.

◆ isx

type(int_bounds_info) m_riemann_state::isx

Definition at line 417 of file m_riemann_state.fpp.f90.

◆ isy

type(int_bounds_info) m_riemann_state::isy

Definition at line 417 of file m_riemann_state.fpp.f90.

◆ isz

type(int_bounds_info) m_riemann_state::isz

Definition at line 417 of file m_riemann_state.fpp.f90.

◆ mom_sp_rsx_vf

real(wp), dimension(:,:,:,:), allocatable m_riemann_state::mom_sp_rsx_vf

Definition at line 388 of file m_riemann_state.fpp.f90.

◆ re_avg_rsx_vf

real(wp), dimension(:,:,:,:), allocatable m_riemann_state::re_avg_rsx_vf

Definition at line 401 of file m_riemann_state.fpp.f90.

◆ res_gs

real(wp), dimension(:,:), allocatable m_riemann_state::res_gs

Definition at line 445 of file m_riemann_state.fpp.f90.

◆ vel_src_rsx_vf

real(wp), dimension(:,:,:,:), allocatable m_riemann_state::vel_src_rsx_vf

Definition at line 375 of file m_riemann_state.fpp.f90.

Functions/Subroutines

Variables

Detailed Description

Function/Subroutine Documentation

◆ s_calculate_bulk_stress_tensor()

◆ s_calculate_shear_stress_tensor()

◆ s_compute_cartesian_viscous_source_flux()

◆ s_compute_cylindrical_viscous_source_flux()

◆ s_compute_viscous_source_flux()

◆ s_finalize_riemann_solver()

◆ s_initialize_riemann_solver()

◆ s_populate_riemann_states_variables_buffers()

Variable Documentation

◆ flux_gsrc_rsx_vf

◆ flux_rsx_vf

◆ flux_src_rsx_vf

◆ gs_rs

◆ is1

◆ is2

◆ is3

◆ isx

◆ isy

◆ isz

◆ mom_sp_rsx_vf

◆ re_avg_rsx_vf

◆ res_gs

◆ vel_src_rsx_vf