Difference between revisions of "Contrib/CompressibleMixingPhaseChangeFoam"

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(Model Equations)
(Model Equations)
Line 5: Line 5:
 
  * Liquid volume transport
 
  * Liquid volume transport
 
Let us consider transport of liquid (heavy phase) volume fraction <math>\alpha_l</math>:
 
Let us consider transport of liquid (heavy phase) volume fraction <math>\alpha_l</math>:
 +
 +
<math>
 +
\frac{\partial \alpha_l \rho_l}{\partial t} + \nabla \cdot
 +
\left (
 +
\right )
 +
</math>
 +
 +
 +
<math>
 +
\frac{\partial{T}}{\partial t} + \nabla \cdot \left(\mathbf{U} T\right) - \nabla \cdot \left( (D_T + \nu_{turb}/Sc_{turb}) \nabla T \right) = 0
 +
</math>
 +
 +
The mass transfer coefficient is determined at each wall by assuming that the value of ''T'' at the wall is zero:
 +
 +
<math>k_c=-\frac{D_T}{T_b} \frac{\partial T}{\partial y}|_{y=0}</math>
 +
 +
where <math>T_b</math> is the bulk value of ''T'' and ''y'' is the direction normal to the wall.
 +
 +
The Sherwood number is then determined by:
 +
 +
<math>Sh=\frac{k_c d}{D_T}</math>
 +
 +
where ''d'' is the characteristic dimension.
 +
 +
In order to use the solver, you should add <math>D_T</math>, <math>T_b</math> and ''d'' to the transportProperties dictionary.
 +
 +
 +
  
 
The solver is based on turbFoam, with the transport of a scalar ''T'' having a mass diffusion coefficient <math>D_T</math>:
 
The solver is based on turbFoam, with the transport of a scalar ''T'' having a mass diffusion coefficient <math>D_T</math>:

Revision as of 19:53, 28 December 2012

Solver for two fluids with phase change (for example - water <---> steam), pressure and temperature density dependence

Model Equations

* Equation of state
* Liquid volume transport

Let us consider transport of liquid (heavy phase) volume fraction \alpha_l:


\frac{\partial \alpha_l \rho_l}{\partial t} + \nabla \cdot 
\left (
\right )


 
\frac{\partial{T}}{\partial t} + \nabla \cdot \left(\mathbf{U} T\right) - \nabla \cdot \left( (D_T + \nu_{turb}/Sc_{turb}) \nabla T \right) = 0

The mass transfer coefficient is determined at each wall by assuming that the value of T at the wall is zero:

k_c=-\frac{D_T}{T_b} \frac{\partial T}{\partial y}|_{y=0}

where T_b is the bulk value of T and y is the direction normal to the wall.

The Sherwood number is then determined by:

Sh=\frac{k_c d}{D_T}

where d is the characteristic dimension.

In order to use the solver, you should add D_T, T_b and d to the transportProperties dictionary.



The solver is based on turbFoam, with the transport of a scalar T having a mass diffusion coefficient D_T:


* Phase change model
* Momentum equation
* Energy equation

Solver sources and tutorials located here