Files | |
cfdivs.f90 | |
cfdttv.f90 | |
cfener.f90 | |
Perform the solving of the convection/diffusion equation (with eventual source terms) for total energy over a time step. It is the third step of the compressible algorithm at each time iteration. | |
cffana.f90 | |
Computes the analytical flux at the boundary for Euler and Energy. | |
cfini1.f90 | |
cfiniv.f90 | |
Initialisation of the variables if the compressible flow model is enabled. | |
cfmsfp.f90 | |
cfmspr.f90 | |
Update the convective mass flux before the velocity prediction step. It is the first step of the compressible algorithm at each time iteration. | |
cfphyv.f90 | |
Computation of variable physical properties for the specific physics compressible. | |
cfpoin.f90 | |
Module for fuel combustion. | |
cfprop.f90 | |
Properties definition initialization for the compressible module, according to calculation type selected by the user. | |
cfrusb.f90 | |
cfvarp.f90 | |
Variables definition initialization for the compressible module, according to calculation type selected by the user. | |
cfxtcl.f90 | |
Handle boundary condition type code (itypfb) when the compressible model is enabled. | |
cs_cf_bindings.f90 | |
Definition of C functions and subroutine bindings for compressible flow module. | |
cs_cf_model.c | |
cs_cf_model.h | |
cs_cf_thermo.c | |
cs_cf_thermo.h | |
cs_cfbl_headers.h | |
cs_hgn_phase_thermo.c | |
Phase thermodynamic for compressible homogeneous two-phase model. | |
cs_hgn_phase_thermo.h | |
cs_hgn_source_terms_step.c | |
Return to equilibrium source terms computation for volume, mass, energy fractions in compressible homogeneous two-phase model. | |
cs_hgn_source_terms_step.h | |
cs_hgn_thermo.c | |
Thermodynamic of a compressible homogeneous two-phase flow. | |
cs_hgn_thermo.h |