programmer's documentation
Variables
Collaboration diagram for Stokes options:

Variables

integer(c_int), pointer, save ivisse
 take $ \divs \left( \mu \transpose{\gradt \, \vect{u}} - 2/3 \mu \trace{\gradt \, \vect{u}} \right) $ into account in the momentum equation More...
 
integer(c_int), pointer, save irevmc
 Reconstruction of the velocity field with the updated pressure option. More...
 
integer(c_int), pointer, save iprco
 Compute the pressure step thanks to the continuity equation. More...
 
integer(c_int), pointer, save irnpnw
 Compute the normed residual for the pressure step in the prediction step. More...
 
real(c_double), pointer, save rnormp
 normed residual for the pressure step More...
 
real(c_double), pointer, save arak
 Arakawa multiplicator for the Rhie and Chow filter (1 by default) More...
 
integer(c_int), pointer, save ipucou
 Pseudo coupled pressure-velocity solver. More...
 
integer(c_int), pointer, save iccvfg
 
integer(c_int), pointer, save idilat
 Algorithm to take into account the density variation in time. More...
 
real(c_double), pointer, save epsdp
 parameter of diagonal pressure strengthening More...
 
integer, dimension(ntypmx), save idebty
 
integer, dimension(ntypmx), save ifinty
 
integer(c_int), pointer, save itbrrb
 accurate treatment of the wall temperature More...
 
integer, dimension(nscamx), save icpsyr
 indicates if the scalar isca is coupled with syrthes More...
 
integer(c_int), pointer, save iphydr
 improve hydrostatic pressure algorithm More...
 
integer(c_int), pointer, save igprij
 improve static pressure algorithm More...
 
integer(c_int), pointer, save igpust
 improve static pressure algorithm More...
 
integer(c_int), pointer, save iifren
 indicates the presence of a Bernoulli boundary face (automatically computed) More...
 
integer(c_int), pointer, save icalhy
 compute the hydrostatic pressure in order to compute the Dirichlet conditions on the pressure at outlets More...
 
integer(c_int), pointer, save irecmf
 use interpolated face diffusion coefficient instead of cell diffusion coefficient for the mass flux reconstruction for the non-orthogonalities More...
 
integer, save icophc
 choice the way to compute the exchange coefficient of the condensation source term used by the copain model More...
 
integer, save icophg
 choice the way to compute the thermal exchange coefficient associated to the heat transfer to wall due to the condensation phenomenon More...
 
integer, save itag1d
 choice the way to compute the wall temperature at the solid/fluid interface coupled with condensation to the wall More...
 
integer, save itagms
 choice the way to compute the wall temperature at the solid/fluid interface coupled with condensation to the metal mass structures wall More...
 
integer, dimension(nestmx), save iescal
 compute error estimators More...
 

Detailed Description

Variable Documentation

real(c_double), pointer, save arak

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

real(c_double), pointer, save epsdp

parameter of diagonal pressure strengthening

integer(c_int), pointer, save icalhy

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

  • 1: true
  • 0: false (default)
integer(c_int), pointer, save iccvfg

calculation with a fixed velocity field

  • 1: true
  • 0: false (default)
integer, save icophc

choice the way to compute the exchange coefficient of the condensation source term used by the copain model

  • 1: the turbulent exchange coefficient of the flow
  • 2: the exchange coefficient of the copain correlation
  • 3: the maximal value between the two previous exchange coefficients
integer, save icophg

choice the way to compute the thermal exchange coefficient associated to the heat transfer to wall due to the condensation phenomenon

  • 2: the thermal exchange coefficient of the copain correlation
  • 3: the maximal value between the current and previous thermal exchange coefficient evaluated by the copain correlation
integer, dimension(nscamx), save icpsyr

indicates if the scalar isca is coupled with syrthes

  • 1: coupled with syrthes
  • 0: uncoupled
Remarks
only one scalar can be coupled with syrthes
integer, dimension(ntypmx), save idebty
integer(c_int), pointer, save 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
integer, dimension(nestmx), save iescal

compute error estimators

  • 1: true
  • 0: false (default)
integer, dimension(ntypmx), save ifinty
integer(c_int), pointer, save igprij

improve static pressure algorithm

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

improve static pressure algorithm

  • 1: take user source term in the static pressure treatment IF iphydr=1 (default)
  • 0: no treatment
integer(c_int), pointer, save iifren

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

  • 0: no face
  • 1: at least one face
integer(c_int), pointer, save iphydr

improve hydrostatic pressure algorithm

  • 1: impose the equilibrium of the hydrostaic part of the pressure with any external force, even head losses
  • 2: compute an hydrostatic pressure due to buoyancy forces before the prediction step
  • 0: no treatment (default)
integer(c_int), pointer, save iprco

Compute the pressure step thanks to the continuity equation.

  • 1: true (default)
  • 0: false
integer(c_int), pointer, save ipucou

Pseudo coupled pressure-velocity solver.

  • 1: true
  • 0: false (default)
integer(c_int), pointer, save 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)
integer(c_int), pointer, save irevmc

Reconstruction of the velocity field with the updated pressure option.

  • 0: default
integer(c_int), pointer, save irnpnw

Compute the normed residual for the pressure step in the prediction step.

  • 1: true (default)
  • 0: false
integer, save itag1d

choice the way to compute the wall temperature at the solid/fluid interface coupled with condensation to the wall

  • 1: the wall temperature is computed with a 1-D thermal model with implicit numerical scheme
  • 0: the wall temperature is imposed as constant by the user (default) exchange coefficient evaluated by the copain correlation
integer, save itagms

choice the way to compute the wall temperature at the solid/fluid interface coupled with condensation to the metal mass structures wall

  • 1: the wall temperature is computed with a 0-D thermal model with explicit numerical scheme
  • 0: the wall temperature is imposed as constant by the user (default) and past to the copain correlation to evaluate the exchange coefficient
integer(c_int), pointer, save itbrrb

accurate treatment of the wall temperature

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

take $ \divs \left( \mu \transpose{\gradt \, \vect{u}} - 2/3 \mu \trace{\gradt \, \vect{u}} \right) $ into account in the momentum equation

  • 1: true (default)
  • 0: false
real(c_double), pointer, save rnormp

normed residual for the pressure step