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MFC
Exascale flow solver
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MFC
Exascale flow solver
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Conservative-to-primitive variable conversion, mixture property evaluation, and pressure computation. More...
Functions/Subroutines | |
| subroutine, public | s_convert_to_mixture_variables (q_vf, i, j, k, rho, gamma, pi_inf, qv, re_k, g_k, g) |
| Dispatch to the s_convert_mixture_to_mixture_variables and s_convert_species_to_mixture_variables subroutines. Replaces a procedure pointer. | |
| subroutine, public | s_compute_pressure (energy, alf, dyn_p, pi_inf, gamma, rho, qv, rhoyks, pres, t, e_e_in, pres_mag) |
| Compute the pressure from the appropriate equation of state. | |
| subroutine, public | s_convert_mixture_to_mixture_variables (q_vf, i, j, k, rho, gamma, pi_inf, qv) |
| Convert mixture variables to density, gamma, pi_inf, and qv for the gamma/pi_inf model. Given conservative or primitive variables, transfers the density, specific heat ratio function and the liquid stiffness function from q_vf to rho, gamma and pi_inf. | |
| subroutine, public | s_convert_species_to_mixture_variables (q_vf, k, l, r, rho, gamma, pi_inf, qv, re_k, g_k, g) |
| Convert species volume fractions and partial densities to mixture density, gamma, pi_inf, and qv. Given conservative or primitive variables, computes the density, the specific heat ratio function and the liquid stiffness function from q_vf and stores the results into rho, gamma and pi_inf. | |
| subroutine, public | s_convert_species_to_mixture_variables_kernel (rho_k, gamma_k, pi_inf_k, qv_k, alpha_k, alpha_rho_k, re_k, g_k, g) |
| Host- and device-callable conversion kernel for species and mixture variables. | |
| impure subroutine, public | s_initialize_variables_conversion_module (store_mixture_fields, enforce_density_floor, preserve_qbmm_number, lagrange_beta_index) |
| Initialize the variables conversion module. | |
| subroutine, public | s_initialize_mv (qk_cons_vf, mv) |
| Initialize bubble mass-vapor values at quadrature nodes from the conserved moment statistics. | |
| subroutine, public | s_initialize_pb (qk_cons_vf, mv, pb) |
| Initialize bubble internal pressures at quadrature nodes using isothermal relations from the Preston model. | |
| subroutine, public | s_convert_conservative_to_primitive_variables (qk_cons_vf, q_t_sf, qk_prim_vf, ibounds) |
| Convert conserved variables (rho*alpha, rho*u, E, alpha) to primitives (rho, u, p, alpha). Conversion depends on model_eqns: each model has different variable sets and EOS. | |
| impure subroutine, public | s_convert_primitive_to_conservative_variables (q_prim_vf, q_cons_vf) |
| Convert primitives (rho, u, p, alpha) to conserved variables (rho*alpha, rho*u, E, alpha). | |
| subroutine, public | s_convert_primitive_to_flux_variables (qk_prim_vf, fk_vf, fk_src_vf, is1, is2, is3, s2b, s3b, dir_idx_in, dir_flg_in, hll_u_interface_in) |
| Convert primitive variables to Eulerian flux variables. | |
| subroutine, public | s_compute_species_fraction (q_vf, k, l, r, alpha_rho_k, alpha_k) |
| Compute partial densities and volume fractions. | |
| impure subroutine, public | s_finalize_variables_conversion_module () |
| Deallocate fluid property arrays and post-processing fields allocated during module initialization. | |
| subroutine, public | s_compute_mixture_coefficients (alpha_rho_k, alpha_k, rho_k, gamma_k, pi_inf_k, qv_k) |
| Mixture coefficients of one state. Under bubbles_euler with num_fluids == 1 the sole advection slot aliases the void fraction (eqn_idxalf == eqn_idxadvend), so alpha is not a composition there and the coefficients are the liquid's. Clipping stays with callers; it differs between solvers and cannot coincide with that case, as mpp_lim requires num_fluids > 1. | |
| subroutine, public | s_compute_mixture_coefficients_dt (dalpha_rho_dt, dadv_dt, drho_dt, dgamma_dt, dpi_inf_dt, dqv_dt) |
| Time derivative of the mixture coefficients, mirroring s_compute_mixture_coefficients. | |
| subroutine, public | s_compute_energy (pres, alpha_rho_k, alpha_k, vel_sum, e) |
| Total energy per unit volume, thermodynamic terms only. Callers add magnetic and elastic energy, which are not equation-of-state terms. The chemistry and relativistic branches use a different relation and stay open-coded. | |
| real(wp) function, public | f_isentrope_exponent (gamma) |
| Exponent of the stiffened-gas isentrope p + B = const rho**n. Precomputed per fluid as isentrope_n. | |
| real(wp) function, public | f_isentrope_pressure (pi_inf, gamma) |
| Reference pressure of that isentrope. Precomputed per fluid as isentrope_B. | |
| real(wp) function, public | f_sg_thermal (pres, rho_or_t, n, b, cv) |
| Stiffened-gas thermal law p + B = (n - 1)*cv*rho*T. Pass rho to get T, or T to get rho. | |
| real(wp) function, public | f_pressure_on_isentrope (pres, xi, n, b) |
| Pressure after isentropic compression from pres through density ratio xi. | |
| real(wp) function, public | f_phase_internal_energy (pres, alpha, alpha_rho, gamma, pi_inf, qv) |
| Internal energy of one six-equation phase: volume-fraction-weighted stiffened-gas energy plus the heat of formation its partial density carries. No kinetic term - that belongs to the mixture, not a phase. | |
| real(wp) function, public | f_elastic_energy (tau, g, is_shear) |
| Elastic strain energy of one stress component, doubled for a shear component: the tensor stores it once, the energy counts both off-diagonal entries. Zero without a shear modulus. | |
| real(wp) function, public | f_hypoelastic_energy (q_cons_vf, j, k, l, rho, g) |
| Hypoelastic strain energy at one cell, summed over the stress components. | |
| real(wp) function, public | f_pressure (e_int, gamma, pi_inf, qv) |
| Pressure of a stiffened gas from its internal energy density - the inverse of s_compute_energy. Callers subtract the kinetic, magnetic and elastic energy first; none of those are equation-of-state terms. | |
| real(wp) function, public | f_bulk_modulus (pres, gamma, pi_inf) |
| Isentropic bulk modulus. Takes coefficients rather than a fluid index, so a mixture - whose effective gamma and pi_inf come from s_compute_mixture_coefficients - is the same call as a single fluid. Elastic callers add their own shear term. | |
| real(wp) function, public | f_relativistic_enthalpy (pres, rho, gamma) |
| Relativistic specific enthalpy, h = 1 + (Gamma + 1)p/rho. Ideal gas only: the stiffness does not appear, so a fluid with a nonzero pi_inf is not represented here (the validator refuses that combination). | |
| subroutine, public | s_compute_speed_of_sound (pres, rho, gamma, pi_inf, adv, c) |
| Speed of sound of a thermodynamic state. Enthalpy is not an argument: for a real state H, |u|^2 and qv all cancel out of c^2 = ((Gamma + 1)p + Pi)/(Gamma rho). Averaged states, whose enthalpy is a free input, use the _avg variant. | |
| subroutine, public | s_compute_speed_of_sound_avg (pres, rho, gamma, pi_inf, qv, vel_sum, h, c_c, adv, c) |
| Speed of sound of an interface-averaged state. An average of two states is not a state - its enthalpy is not the one its pressure and density imply - so the caller supplies H, |u|^2 and qv. Only the enthalpy-reading branches differ from s_compute_speed_of_sound; keep the condition below in step with the branch list there. | |
| subroutine, public | s_compute_fast_magnetosonic_speed (rho, c, b, norm, c_fast, h) |
| Compute the fast magnetosonic wave speed from the sound speed, density, and magnetic field components. | |
Variables | |
| real(wp), dimension(:), allocatable | gs_vc |
| integer, dimension(:), allocatable | bubrs_vc |
| real(wp), dimension(:,:), allocatable | res_vc |
| integer | is1b |
| integer | is2b |
| integer | is3b |
| integer | is1e |
| integer | is2e |
| integer | is3e |
| logical | enforce_density_floor_vc = .false. |
| logical | preserve_qbmm_number_vc = .false. |
| integer | lagrange_beta_index_vc = 0 |
| real(wp), dimension(:,:,:), allocatable, public | rho_sf |
| Scalar density function. | |
| real(wp), dimension(:,:,:), allocatable, public | gamma_sf |
| Scalar sp. heat ratio function. | |
| real(wp), dimension(:,:,:), allocatable, public | pi_inf_sf |
| Scalar liquid stiffness function. | |
Conservative-to-primitive variable conversion, mixture property evaluation, and pressure computation.
| real(wp) function, public m_variables_conversion::f_bulk_modulus | ( | real(wp), intent(in) | pres, |
| real(wp), intent(in) | gamma, | ||
| real(wp), intent(in) | pi_inf ) |
Isentropic bulk modulus. Takes coefficients rather than a fluid index, so a mixture - whose effective gamma and pi_inf come from s_compute_mixture_coefficients - is the same call as a single fluid. Elastic callers add their own shear term.
Definition at line 3074 of file m_variables_conversion.fpp.f90.
| real(wp) function, public m_variables_conversion::f_elastic_energy | ( | real(wp), intent(in) | tau, |
| real(wp), intent(in) | g, | ||
| logical, intent(in) | is_shear ) |
Elastic strain energy of one stress component, doubled for a shear component: the tensor stores it once, the energy counts both off-diagonal entries. Zero without a shear modulus.
Definition at line 2959 of file m_variables_conversion.fpp.f90.
| real(wp) function, public m_variables_conversion::f_hypoelastic_energy | ( | type(scalar_field), dimension(sys_size), intent(in) | q_cons_vf, |
| integer, intent(in) | j, | ||
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| real(wp), intent(in) | rho, | ||
| real(wp), intent(in) | g ) |
Hypoelastic strain energy at one cell, summed over the stress components.
Definition at line 3010 of file m_variables_conversion.fpp.f90.
| real(wp) function, public m_variables_conversion::f_isentrope_exponent | ( | real(wp), intent(in) | gamma | ) |
Exponent of the stiffened-gas isentrope p + B = const rho**n. Precomputed per fluid as isentrope_n.
Definition at line 2727 of file m_variables_conversion.fpp.f90.
| real(wp) function, public m_variables_conversion::f_isentrope_pressure | ( | real(wp), intent(in) | pi_inf, |
| real(wp), intent(in) | gamma ) |
Reference pressure of that isentrope. Precomputed per fluid as isentrope_B.
Definition at line 2773 of file m_variables_conversion.fpp.f90.
| real(wp) function, public m_variables_conversion::f_phase_internal_energy | ( | real(wp), intent(in) | pres, |
| real(wp), intent(in) | alpha, | ||
| real(wp), intent(in) | alpha_rho, | ||
| real(wp), intent(in) | gamma, | ||
| real(wp), intent(in) | pi_inf, | ||
| real(wp), intent(in) | qv ) |
Internal energy of one six-equation phase: volume-fraction-weighted stiffened-gas energy plus the heat of formation its partial density carries. No kinetic term - that belongs to the mixture, not a phase.
Definition at line 2912 of file m_variables_conversion.fpp.f90.
| real(wp) function, public m_variables_conversion::f_pressure | ( | real(wp), intent(in) | e_int, |
| real(wp), intent(in) | gamma, | ||
| real(wp), intent(in) | pi_inf, | ||
| real(wp), intent(in) | qv ) |
Pressure of a stiffened gas from its internal energy density - the inverse of s_compute_energy. Callers subtract the kinetic, magnetic and elastic energy first; none of those are equation-of-state terms.
Definition at line 3027 of file m_variables_conversion.fpp.f90.
| real(wp) function, public m_variables_conversion::f_pressure_on_isentrope | ( | real(wp), intent(in) | pres, |
| real(wp), intent(in) | xi, | ||
| real(wp), intent(in) | n, | ||
| real(wp), intent(in) | b ) |
Pressure after isentropic compression from pres through density ratio xi.
Definition at line 2865 of file m_variables_conversion.fpp.f90.
| real(wp) function, public m_variables_conversion::f_relativistic_enthalpy | ( | real(wp), intent(in) | pres, |
| real(wp), intent(in) | rho, | ||
| real(wp), intent(in) | gamma ) |
Relativistic specific enthalpy, h = 1 + (Gamma + 1)p/rho. Ideal gas only: the stiffness does not appear, so a fluid with a nonzero pi_inf is not represented here (the validator refuses that combination).
Definition at line 3121 of file m_variables_conversion.fpp.f90.
| real(wp) function, public m_variables_conversion::f_sg_thermal | ( | real(wp), intent(in) | pres, |
| real(wp), intent(in) | rho_or_t, | ||
| real(wp), intent(in) | n, | ||
| real(wp), intent(in) | b, | ||
| real(wp), intent(in) | cv ) |
Stiffened-gas thermal law p + B = (n - 1)*cv*rho*T. Pass rho to get T, or T to get rho.
Definition at line 2819 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_compute_energy | ( | real(wp), intent(in) | pres, |
| real(wp), dimension(num_fluids), intent(in) | alpha_rho_k, | ||
| real(wp), dimension(num_fluids), intent(in) | alpha_k, | ||
| real(wp), intent(in) | vel_sum, | ||
| real(wp), intent(out) | e ) |
Total energy per unit volume, thermodynamic terms only. Callers add magnetic and elastic energy, which are not equation-of-state terms. The chemistry and relativistic branches use a different relation and stay open-coded.
Definition at line 2671 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_compute_fast_magnetosonic_speed | ( | real(wp), intent(in) | rho, |
| real(wp), intent(in) | c, | ||
| real(wp), dimension(3), intent(in) | b, | ||
| integer, intent(in) | norm, | ||
| real(wp), intent(out) | c_fast, | ||
| real(wp), intent(in) | h ) |
Compute the fast magnetosonic wave speed from the sound speed, density, and magnetic field components.
| [in] | h | only used for relativity |
Definition at line 3292 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_compute_mixture_coefficients | ( | real(wp), dimension(num_fluids), intent(in) | alpha_rho_k, |
| real(wp), dimension(num_fluids), intent(in) | alpha_k, | ||
| real(wp), intent(out) | rho_k, | ||
| real(wp), intent(out) | gamma_k, | ||
| real(wp), intent(out) | pi_inf_k, | ||
| real(wp), intent(out) | qv_k ) |
Mixture coefficients of one state. Under bubbles_euler with num_fluids == 1 the sole advection slot aliases the void fraction (eqn_idxalf == eqn_idxadvend), so alpha is not a composition there and the coefficients are the liquid's. Clipping stays with callers; it differs between solvers and cannot coincide with that case, as mpp_lim requires num_fluids > 1.
Definition at line 2512 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_compute_mixture_coefficients_dt | ( | real(wp), dimension(num_fluids), intent(in) | dalpha_rho_dt, |
| real(wp), dimension(num_fluids), intent(in) | dadv_dt, | ||
| real(wp), intent(out) | drho_dt, | ||
| real(wp), intent(out) | dgamma_dt, | ||
| real(wp), intent(out) | dpi_inf_dt, | ||
| real(wp), intent(out) | dqv_dt ) |
Time derivative of the mixture coefficients, mirroring s_compute_mixture_coefficients.
Definition at line 2594 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_compute_pressure | ( | real(stp), intent(in) | energy, |
| real(stp), intent(in) | alf, | ||
| real(wp), intent(in) | dyn_p, | ||
| real(wp), intent(in) | pi_inf, | ||
| real(wp), intent(in) | gamma, | ||
| real(wp), intent(in) | rho, | ||
| real(wp), intent(in) | qv, | ||
| real(wp), dimension(1:num_species), intent(in) | rhoyks, | ||
| real(wp), intent(out) | pres, | ||
| real(wp), intent(inout) | t, | ||
| real(wp), intent(in), optional | e_e_in, | ||
| real(wp), intent(in), optional | pres_mag ) |
Compute the pressure from the appropriate equation of state.
Definition at line 428 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_compute_species_fraction | ( | type(scalar_field), dimension(sys_size), intent(in) | q_vf, |
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| integer, intent(in) | r, | ||
| real(wp), dimension(num_fluids), intent(out) | alpha_rho_k, | ||
| real(wp), dimension(num_fluids), intent(out) | alpha_k ) |
Compute partial densities and volume fractions.
Definition at line 2322 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_compute_speed_of_sound | ( | real(wp), intent(in) | pres, |
| real(wp), intent(in) | rho, | ||
| real(wp), intent(in) | gamma, | ||
| real(wp), intent(in) | pi_inf, | ||
| real(wp), dimension(num_fluids), intent(in) | adv, | ||
| real(wp), intent(out) | c ) |
Speed of sound of a thermodynamic state. Enthalpy is not an argument: for a real state H, |u|^2 and qv all cancel out of c^2 = ((Gamma + 1)p + Pi)/(Gamma rho). Averaged states, whose enthalpy is a free input, use the _avg variant.
Definition at line 3168 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_compute_speed_of_sound_avg | ( | real(wp), intent(in) | pres, |
| real(wp), intent(in) | rho, | ||
| real(wp), intent(in) | gamma, | ||
| real(wp), intent(in) | pi_inf, | ||
| real(wp), intent(in) | qv, | ||
| real(wp), intent(in) | vel_sum, | ||
| real(wp), intent(in) | h, | ||
| real(wp), intent(in) | c_c, | ||
| real(wp), dimension(num_fluids), intent(in) | adv, | ||
| real(wp), intent(out) | c ) |
Speed of sound of an interface-averaged state. An average of two states is not a state - its enthalpy is not the one its pressure and density imply - so the caller supplies H, |u|^2 and qv. Only the enthalpy-reading branches differ from s_compute_speed_of_sound; keep the condition below in step with the branch list there.
Definition at line 3245 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_convert_conservative_to_primitive_variables | ( | type(scalar_field), dimension(sys_size), intent(in) | qk_cons_vf, |
| type(scalar_field), intent(inout) | q_t_sf, | ||
| type(scalar_field), dimension(sys_size), intent(inout) | qk_prim_vf, | ||
| type(int_bounds_info), dimension(1:3), intent(in) | ibounds ) |
Convert conserved variables (rho*alpha, rho*u, E, alpha) to primitives (rho, u, p, alpha). Conversion depends on model_eqns: each model has different variable sets and EOS.
Definition at line 1215 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_convert_mixture_to_mixture_variables | ( | type(scalar_field), dimension(sys_size), intent(in) | q_vf, |
| integer, intent(in) | i, | ||
| integer, intent(in) | j, | ||
| integer, intent(in) | k, | ||
| real(wp), intent(out), target | rho, | ||
| real(wp), intent(out), target | gamma, | ||
| real(wp), intent(out), target | pi_inf, | ||
| real(wp), intent(out), target | qv ) |
Convert mixture variables to density, gamma, pi_inf, and qv for the gamma/pi_inf model. Given conservative or primitive variables, transfers the density, specific heat ratio function and the liquid stiffness function from q_vf to rho, gamma and pi_inf.
Definition at line 506 of file m_variables_conversion.fpp.f90.
| impure subroutine, public m_variables_conversion::s_convert_primitive_to_conservative_variables | ( | type(scalar_field), dimension(sys_size), intent(in) | q_prim_vf, |
| type(scalar_field), dimension(sys_size), intent(inout) | q_cons_vf ) |
Convert primitives (rho, u, p, alpha) to conserved variables (rho*alpha, rho*u, E, alpha).
Definition at line 1732 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_convert_primitive_to_flux_variables | ( | real(wp), dimension(0:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:), intent(in) | qk_prim_vf, |
| real(wp), dimension(0:,idwbuff(2)%beg:,idwbuff(3)%beg:,1:), intent(inout) | fk_vf, | ||
| real(wp), dimension(0:,idwbuff(2)%beg:,idwbuff(3)%beg:,eqn_idx%adv%beg:), intent(inout) | fk_src_vf, | ||
| type(int_bounds_info), intent(in) | is1, | ||
| type(int_bounds_info), intent(in) | is2, | ||
| type(int_bounds_info), intent(in) | is3, | ||
| integer, intent(in) | s2b, | ||
| integer, intent(in) | s3b, | ||
| integer, dimension(3), intent(in) | dir_idx_in, | ||
| real(wp), dimension(3), intent(in) | dir_flg_in, | ||
| logical, intent(in) | hll_u_interface_in ) |
Convert primitive variables to Eulerian flux variables.
| [in] | dir_idx_in | Working-direction mapping, passed explicitly: it is simulation state (m_global_parameters), and use-associating it into this common kernel spills registers on AMD OpenMP offload. |
Definition at line 1962 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_convert_species_to_mixture_variables | ( | type(scalar_field), dimension(sys_size), intent(in) | q_vf, |
| integer, intent(in) | k, | ||
| integer, intent(in) | l, | ||
| integer, intent(in) | r, | ||
| real(wp), intent(out), target | rho, | ||
| real(wp), intent(out), target | gamma, | ||
| real(wp), intent(out), target | pi_inf, | ||
| real(wp), intent(out), target | qv, | ||
| real(wp), dimension(2), intent(out), optional | re_k, | ||
| real(wp), intent(out), optional | g_k, | ||
| real(wp), dimension(num_fluids), intent(in), optional | g ) |
Convert species volume fractions and partial densities to mixture density, gamma, pi_inf, and qv. Given conservative or primitive variables, computes the density, the specific heat ratio function and the liquid stiffness function from q_vf and stores the results into rho, gamma and pi_inf.
Definition at line 534 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_convert_species_to_mixture_variables_kernel | ( | real(wp), intent(out) | rho_k, |
| real(wp), intent(out) | gamma_k, | ||
| real(wp), intent(out) | pi_inf_k, | ||
| real(wp), intent(out) | qv_k, | ||
| real(wp), dimension(num_fluids), intent(inout) | alpha_k, | ||
| real(wp), dimension(num_fluids), intent(inout) | alpha_rho_k, | ||
| real(wp), dimension(2), intent(out), optional | re_k, | ||
| real(wp), intent(out), optional | g_k, | ||
| real(wp), dimension(num_fluids), intent(in), optional | g ) |
Host- and device-callable conversion kernel for species and mixture variables.
Definition at line 565 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_convert_to_mixture_variables | ( | type(scalar_field), dimension(sys_size), intent(in) | q_vf, |
| integer, intent(in) | i, | ||
| integer, intent(in) | j, | ||
| integer, intent(in) | k, | ||
| real(wp), intent(out), target | rho, | ||
| real(wp), intent(out), target | gamma, | ||
| real(wp), intent(out), target | pi_inf, | ||
| real(wp), intent(out), target | qv, | ||
| real(wp), dimension(2), intent(out), optional | re_k, | ||
| real(wp), intent(out), optional | g_k, | ||
| real(wp), dimension(num_fluids), intent(in), optional | g ) |
Dispatch to the s_convert_mixture_to_mixture_variables and s_convert_species_to_mixture_variables subroutines. Replaces a procedure pointer.
Definition at line 410 of file m_variables_conversion.fpp.f90.
| impure subroutine, public m_variables_conversion::s_finalize_variables_conversion_module |
Deallocate fluid property arrays and post-processing fields allocated during module initialization.
Definition at line 2405 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_initialize_mv | ( | type(scalar_field), dimension(sys_size), intent(in) | qk_cons_vf, |
| real(stp), dimension(idwint(1)%beg:,idwint(2)%beg:,idwint(3)%beg:,1:,1:), intent(inout) | mv ) |
Initialize bubble mass-vapor values at quadrature nodes from the conserved moment statistics.
Definition at line 1130 of file m_variables_conversion.fpp.f90.
| subroutine, public m_variables_conversion::s_initialize_pb | ( | type(scalar_field), dimension(sys_size), intent(in) | qk_cons_vf, |
| real(stp), dimension(idwint(1)%beg:,idwint(2)%beg:,idwint(3)%beg:,1:,1:), intent(in) | mv, | ||
| real(stp), dimension(idwint(1)%beg:,idwint(2)%beg:,idwint(3)%beg:,1:,1:), intent(inout) | pb ) |
Initialize bubble internal pressures at quadrature nodes using isothermal relations from the Preston model.
Definition at line 1169 of file m_variables_conversion.fpp.f90.
| impure subroutine, public m_variables_conversion::s_initialize_variables_conversion_module | ( | logical, intent(in), optional | store_mixture_fields, |
| logical, intent(in), optional | enforce_density_floor, | ||
| logical, intent(in), optional | preserve_qbmm_number, | ||
| integer, intent(in), optional | lagrange_beta_index ) |
Initialize the variables conversion module.
Definition at line 658 of file m_variables_conversion.fpp.f90.
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Definition at line 360 of file m_variables_conversion.fpp.f90.
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Definition at line 387 of file m_variables_conversion.fpp.f90.
| real(wp), dimension(:,:,:), allocatable, public m_variables_conversion::gamma_sf |
Scalar sp. heat ratio function.
Definition at line 403 of file m_variables_conversion.fpp.f90.
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Definition at line 359 of file m_variables_conversion.fpp.f90.
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Definition at line 374 of file m_variables_conversion.fpp.f90.
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Definition at line 374 of file m_variables_conversion.fpp.f90.
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Definition at line 374 of file m_variables_conversion.fpp.f90.
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Definition at line 374 of file m_variables_conversion.fpp.f90.
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Definition at line 374 of file m_variables_conversion.fpp.f90.
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Definition at line 374 of file m_variables_conversion.fpp.f90.
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Definition at line 389 of file m_variables_conversion.fpp.f90.
| real(wp), dimension(:,:,:), allocatable, public m_variables_conversion::pi_inf_sf |
Scalar liquid stiffness function.
Definition at line 404 of file m_variables_conversion.fpp.f90.
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Definition at line 388 of file m_variables_conversion.fpp.f90.
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Definition at line 361 of file m_variables_conversion.fpp.f90.
| real(wp), dimension(:,:,:), allocatable, public m_variables_conversion::rho_sf |
Scalar density function.
Definition at line 402 of file m_variables_conversion.fpp.f90.