|  | programmer's documentation | 
| 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
 1.8.3.1