Difference between revisions of "Contrib/CompressibleMixingPhaseChangeFoam"

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(Model Equations)
(Model Equations)
Line 17: Line 17:
  
 
where <math>\hat \rho</math> computed with respect to previous formulations
 
where <math>\hat \rho</math> computed with respect to previous formulations
 +
 +
 +
mixture density <math> \rho </math> calculated as
 +
 +
<math>\rho =  \alpha_l \rho_l + \alpha_v \rho_v </math>
 +
 
* 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>:
Line 63: Line 69:
 
\zeta \alpha_l \frac {d \rho_i}{dt}  + \zeta \rho_i \frac {d \alpha_i}{dt}
 
\zeta \alpha_l \frac {d \rho_i}{dt}  + \zeta \rho_i \frac {d \alpha_i}{dt}
 
</math>
 
</math>
 +
 +
* Momentum equation (velocity prediction)
 +
\frac {\partial \rho \textbf{U}}{\partial t}
  
 
  * Phase change model
 
  * Phase change model
* Momentum equation
 
 
  * Energy equation
 
  * Energy equation
 
[http://www.os-cfd.ru/compressibleMixingPhaseChangeFoam/Solver.tgz Solver sources and tutorials located here]
 
[http://www.os-cfd.ru/compressibleMixingPhaseChangeFoam/Solver.tgz Solver sources and tutorials located here]

Revision as of 20:54, 28 December 2012

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

Model Equations

  • Equation of state

Low-compressible fluid: 
\rho = \rho_0 + \frac{\partial \rho}{\partial T} \Delta T + \frac{\partial \rho}{\partial p} \Delta p

Ideal gas:  \rho=\frac{p}{(C_p/C_v)(R/M)T}

By combining this equations, we can get general relation:


\rho = \hat \rho + \frac{\partial \rho}{\partial p} \Delta p

where \hat \rho computed with respect to previous formulations


mixture density  \rho calculated as

\rho =  \alpha_l \rho_l + \alpha_v \rho_v

  • 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 (
  \alpha_l \rho_l \mathbf{U}
\right )
=
\dot m_l


By converting to volume fluxes we get:


\frac {\partial \alpha_l}{\partial t} + \nabla \cdot
\left (
 \alpha_l \textbf{U}
\right )
= \frac {\alpha_l}{\rho_l} \frac {d \rho_l}{dt} + \frac {\dot m_l}{\rho_l}

Using equation of state, we can reformulate substantial derivative for density in terms of pressure for any phase:


\frac {d \rho}{dt}= \frac {d \hat \rho} {dt}
 + \psi \frac {dp} {dt}
 + p \frac {d \psi}{dt}

  • General rule for converting from mass to volume fluxes in transport equation


\frac{\partial \alpha_i \rho_i \zeta}{\partial t}
+
\nabla \cdot 
\left (
\alpha_i \rho_i \textbf{U} \zeta
\right )
= \rho_i \alpha_i 
\left (
 \frac {\partial \zeta}{\partial t} + \nabla \cdot \left ( \textbf{U} \zeta \right )
\right )
+
\zeta \alpha_l \frac {d \rho_i}{dt}  + \zeta \rho_i \frac {d \alpha_i}{dt}

  • Momentum equation (velocity prediction)

\frac {\partial \rho \textbf{U}}{\partial t}

* Phase change model
* Energy equation

Solver sources and tutorials located here