Différences

Ci-dessous, les différences entre deux révisions de la page.

--- sunfluidh:new_numerical_methods_setup_namelist [2017/09/25 14:07] – [Namelist Numerical_Methods (new version)] yann
+++ sunfluidh:new_numerical_methods_setup_namelist [2017/09/25 14:33] – [Full data set of the namelist] yann
@@ Ligne 30: / Ligne 30: @@
    * The partial diagonalization method (Poisson_NumericalMethod = "Home-PartialDiagonalization") used for solving the Poisson equation is only permitted for separable problems.
    * The HYPRE library solvers for solving the Poisson's equation are only available if the HYPRE library has been installed.
 </note>
@@ Ligne 39: / Ligne 40: @@
 -----
 ====  NS_NumericalMethod  ====
-(equivalent to "Numerical_Scheme" in the previous release)
+(equivalent to "Numerical_Scheme" in the previous release, see [[Numerical_Methods_Setup_Namelist |Numerical_Methods (old version)]] )
    * Type: character string
    * Selection of the numerical scheme for solving the conservation equations :
@@ Ligne 54: / Ligne 55: @@
 ==== MomentumConvection_Scheme ====
-(equivalent to "Convective_Flux_Discretization_Type" in the previous release)
+(equivalent to "Convective_Flux_Discretization_Type" in the previous release, see [[Numerical_Methods_Setup_Namelist |Numerical_Methods (old version)]] )
    * Type : character string
    * Selection of the 2nd order spatial discretization for the convection flux in the momentum equations. The options are :
@@ Ligne 90: / Ligne 91: @@
 ====  Poisson_NumericalMethod ====
-(equivalent to "Numerical_Method_Poisson_Equation " in the previous release)
+(equivalent to "Numerical_Method_Poisson_Equation " in the previous release, see [[Numerical_Methods_Setup_Namelist |Numerical_Methods (old version)]] )
    * Type : Character string
    * Selection of the numerical method for solving the Poisson equation in accordance to the projection method. The solution is the pressure time increment ($\Phi= P^{n+1}-P^{n}$, Goda's method) used to update the velocity field according to the principle of the projection method (When the numerical method of Njam et al. is used to solve the Navier-Stokes equations, the pressure is solved in place of its time increment (Chorin's method). The options are :