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programmer's documentation
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Files | |
| file | bilsc4.f90 |
This function adds the explicit part of the convection/diffusion terms of a transport equation of a vector field . | |
| file | bilsca.f90 |
Wrapper to the function which adds the explicit part of the convection/diffusion terms of a transport equation of a scalar field . | |
| file | bilsct.f90 |
This function adds the explicit part of the convection/diffusion terms of a transport equation of a scalar field such as the temperature. | |
| file | bilscv.f90 |
Wrapper to the function which adds the explicit part of the convection/diffusion terms of a transport equation of a vector field . | |
| file | cs_benchmark.c |
| file | cs_benchmark.h [code] |
| file | cs_blas.c |
| file | cs_blas.h [code] |
| file | cs_convection_diffusion_balance.c |
| file | cs_convection_diffusion_balance.h [code] |
| file | cs_gradient.c |
| file | cs_gradient.h [code] |
| file | cs_gradient_perio.c |
| file | cs_gradient_perio.h [code] |
| file | cs_grid.c |
| file | cs_grid.h [code] |
| file | cs_matrix.c |
| file | cs_matrix.h [code] |
| file | cs_matrix_priv.h [code] |
| file | cs_matrix_util.c |
| file | cs_matrix_util.h [code] |
| file | cs_multigrid.c |
| file | cs_multigrid.h [code] |
| file | cs_sles.c |
| file | cs_sles.h [code] |
| file | diften.f90 |
This function adds the explicit part of the diffusion terms with a symmetric tensor diffusivity for a transport equation of a scalar field . | |
| file | diftnv.f90 |
This function adds the explicit part of the diffusion terms with a symmetric tensor diffusivity for a transport equation of a vector field . | |
| file | divmas.f90 |
| file | divrij.f90 |
| file | grdcel.f90 |
| file | grdpot.f90 |
| file | grdpre.f90 |
| file | grdvec.f90 |
| file | inimas.f90 |
This function adds to the mass flux for the segregated algorithm on the velocity components. | |
| file | inimav.f90 |
this function adds to the mass flux . | |
| file | invers.f90 |
| file | itrgrp.f90 |
| file | itrgrv.f90 |
| This function adds the explicit part of the divergence of the mass flux due to the pressure gradient (routine analog to diften.f90). | |
| file | itrmas.f90 |
| file | itrmav.f90 |
This function adds the explicit part of the pressure gradient to the mass flux for a tensorial diffusion for the pressure field . | |
| file | matrdt.f90 |
| file | matrix.f90 |
| This function builds the matrix of advection/diffusion for a scalar field. | |
| file | matrvv.f90 |
| This function builds the matrix of advection/diffusion for a vector field with a tensorial diffusivity. | |
| file | matrxv.f90 |
| This function builds the matrix of advection/diffusion for a vector field. | |
| file | prodsc.f90 |
Dot product vava = . | |
| file | projts.f90 |
| file | projtv.f90 |
| This function projects the external source termes to the faces in coherence with itrmav.f90 for the improved hydrostatic pressure algorithm (iphydr=1). | |
| file | viscfa.f90 |
| file | visort.f90 |
| file | vistnv.f90 |
| This function computes the equivalent tensor viscosity at faces for a 3x3 symetric tensor. | |
| file | vitens.f90 |
| This function computes the equivalent viscosity at faces for a 3x3 symetric tensor. | |
1.8.3.1