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MFC
Exascale flow solver
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Contains module m_derived_variables. More...
Go to the source code of this file.
Modules | |
| module | m_derived_variables |
| Computes derived flow quantities (sound speed, vorticity, Schlieren, etc.) from conservative and primitive variables. | |
Functions/Subroutines | |
| impure subroutine, public | m_derived_variables::s_initialize_derived_variables_module |
| Computation of parameters, allocation procedures, and/or any other tasks needed to properly setup the module. | |
| subroutine, public | m_derived_variables::s_derive_specific_heat_ratio (q_sf) |
| Derive the specific heat ratio from the specific heat ratio function gamma_sf. The latter is stored in the derived flow quantity storage variable, q_sf. | |
| subroutine, public | m_derived_variables::s_derive_liquid_stiffness (q_sf) |
| Compute the liquid stiffness from the specific heat ratio function gamma_sf and the liquid stiffness function pi_inf_sf, respectively. These are used to calculate the values of the liquid stiffness, which are stored in the derived flow quantity storage variable, q_sf. | |
| subroutine, public | m_derived_variables::s_derive_sound_speed (q_prim_vf, q_sf) |
| Compute the speed of sound from the primitive variables, density, specific heat ratio function, and liquid stiffness function. It then computes from those variables the values of the speed of sound, which are stored in the derived flow quantity storage variable, q_sf. | |
| subroutine, public | m_derived_variables::s_derive_flux_limiter (i, q_prim_vf, q_sf) |
| Derive the flux limiter at cell boundary i+1/2. This is an approximation because the velocity used to determine the upwind direction is the velocity at the cell center i instead of the contact velocity at the cell boundary from the Riemann solver. | |
| subroutine | m_derived_variables::s_solve_linear_system (a, b, sol, ndim) |
| Solve Ax=b via Gaussian elimination with partial pivoting. | |
| subroutine, public | m_derived_variables::s_derive_vorticity_component (i, q_prim_vf, q_sf) |
| Compute the specified component of the vorticity from the primitive variables. From those inputs, it proceeds to calculate values of the desired vorticity component, which are subsequently stored in derived flow quantity storage variable, q_sf. | |
| subroutine, public | m_derived_variables::s_derive_qm (q_prim_vf, q_sf) |
| Compute the Q_M criterion from the primitive variables. The Q_M function, which are subsequently stored in the derived flow quantity storage variable, q_sf. | |
| impure subroutine, public | m_derived_variables::s_derive_liutex (q_prim_vf, liutex_mag, liutex_axis) |
| Compute the Liutex vector and its magnitude based on Xu et al. (2019). | |
| impure subroutine, public | m_derived_variables::s_derive_numerical_schlieren_function (q_cons_vf, q_sf) |
| Compute the values of the numerical Schlieren function, which are subsequently stored in the derived flow quantity storage variable, q_sf. | |
| impure subroutine, public | m_derived_variables::s_finalize_derived_variables_module |
| Deallocation procedures for the module. | |
Variables | |
| real(wp), dimension(:,:,:), allocatable | m_derived_variables::gm_rho_sf |
| Density gradient magnitude for numerical Schlieren. | |
| integer, private | m_derived_variables::flg |
| Dimensionality flag: 1 = 3D dataset, 0 = otherwise. | |
Finite-difference (fd) coefficients in x-, y- and z-coordinate directions. Note that because sufficient boundary | |
information is available for all the active coordinate directions, the centered family of the finite-difference schemes is used. | |
| real(wp), dimension(:,:), allocatable, public | m_derived_variables::fd_coeff_x |
| real(wp), dimension(:,:), allocatable, public | m_derived_variables::fd_coeff_y |
| real(wp), dimension(:,:), allocatable, public | m_derived_variables::fd_coeff_z |
Contains module m_derived_variables.
Definition in file m_derived_variables.fpp.f90.