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cs_stokes_model_t Struct Reference

Stokes equation model descriptor. More...

#include <cs_stokes_model.h>

Collaboration diagram for cs_stokes_model_t:
Collaboration graph

Data Fields

int ivisse
 
int irevmc
 
int iprco
 
int irnpnw
 
double rnormp
 
double arak
 
int ipucou
 
int iccvfg
 
int idilat
 
double epsdp
 
int itbrrb
 
int iphydr
 
int igprij
 
int igpust
 
int iifren
 
int icalhy
 
int irecmf
 

Detailed Description

Stokes equation model descriptor.

Members of these Stokes equation model descriptor are publicly accessible, to allow for concise syntax, as it is expected to be used in many places.

Field Documentation

arak

Arakawa multiplicator for the Rhie and Chow filter (1 by default)

epsdp

parameter of diagonal pressure strengthening

icalhy

compute the hydrostatic pressure in order to compute the Dirichlet conditions on the pressure at outlets

  • 1: true
  • 0: false (default)
iccvfg

calculation with a fixed velocity field

  • 1: true
  • 0: false (default)
idilat

algorithm to take into account the density variation in time

  • 1: dilatable steady algorithm (default)
  • 2: dilatable unsteady algorithm
  • 3: low-Mach algorithm
  • 4: algorithm for fire
igprij

improve static pressure algorithm

  • 1: take -div(rho R) in the static pressure treatment IF iphydr=1
  • 0: no treatment (default)
igpust

improve static pressure algorithm

  • 1: take user momentum source terms in the static pressure treatment IF iphydr=1
  • 0: no treatment (default)
iifren

indicates the presence of a Bernoulli boundary face (automatically computed)

  • 0: no face
  • 1: at least one face
iphydr

improve static pressure algorithm Take into account the balance or imbalance between the pressure gradient and source terms (as gravity and head losses)

  • 1: impose the equilibrium of the hydrostaic part of the pressure with any external force, even head losses
  • 0: no treatment (default)
  • 2: hydrostatic pressure computation with a apriori momentum equation to obtain a hydrostatic pressure taking into account the imbalance between the pressure gradient and the gravity source term
iprco

compute the pressure step thanks to the continuity equation

  • 1: true (default)
  • 0: false
ipucou

pseudo coupled pressure-velocity solver

  • 1: true (default)
  • 0: false
irecmf

use interpolated face diffusion coefficient instead of cell diffusion coefficient for the mass flux reconstruction for the non-orthogonalities

  • 1: true
  • 0: false (default)
irevmc

reconstruction of the velocity field with the updated pressure option

  • 0: default
irnpnw

compute the normed residual for the pressure step in the prediction step

  • 1: true (default)
  • 0: false
itbrrb

accurate treatment of the wall temperature (reconstruction of wall temperature)

  • 1: true
  • 0: false (default) (see condli, useful in case of coupling with syrthes)
ivisse

take $ \divs \left( \mu \transpose{\gradt \, \vect{u}} - 2/3 \mu \trace{\gradt \, \vect{u}} \right) $

rnormp

normed residual for the pressure step


The documentation for this struct was generated from the following files: