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file | cfdivs.f90 |
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file | cfdttv.f90 |
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file | 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.
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file | cffana.f90 |
| Computes the analytical flux at the boundary for Euler and Energy.
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file | cfini1.f90 |
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file | cfiniv.f90 |
| Initialisation of the variables if the compressible flow model is enabled.
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file | cfmsfp.f90 |
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file | 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.
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file | cfphyv.f90 |
| Computation of variable physical properties for the specific physics compressible.
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file | cfpoin.f90 |
| Module for fuel combustion.
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file | cfprop.f90 |
| Properties definition initialization for the compressible module, according to calculation type selected by the user.
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file | cfrusb.f90 |
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file | cfvarp.f90 |
| Variables definition initialization for the compressible module, according to calculation type selected by the user.
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file | cfxtcl.f90 |
| Handle boundary condition type code (itypfb) when the compressible model is enabled.
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file | cs_cf_bindings.f90 |
| Definition of C functions and subroutine bindings for compressible flow module.
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file | cs_cf_model.c |
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file | cs_cf_model.h [code] |
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file | cs_cf_thermo.c |
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file | cs_cf_thermo.h [code] |
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file | cs_hgn_phase_thermo.c |
| Phase thermodynamic for compressible homogeneous two-phase model.
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file | cs_hgn_phase_thermo.h [code] |
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file | cs_hgn_source_terms_step.c |
| Return to equilibrium source terms computation for volume, mass, energy fractions in compressible homogeneous two-phase model.
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file | cs_hgn_source_terms_step.h [code] |
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file | cs_hgn_thermo.c |
| Thermodynamic of a compressible homogeneous two-phase flow.
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file | cs_hgn_thermo.h [code] |
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