Difference between revisions of "Contrib/CompressibleMixingPhaseChangeFoam"
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== Model Equations == | == Model Equations == | ||
* Equation of state | * Equation of state | ||
− | Low-compressible fluid: \rho = \rho_0 + \frac{\partial \rho}{\partial T} \ | + | Low-compressible fluid: <math> |
+ | \rho = \rho_0 + \frac{\partial \rho}{\partial T} \Delta T + \frac{\partial \rho}{\partial p} \Delta p | ||
+ | </math> | ||
+ | |||
+ | Ideal gas: <math> \rho=\frac{p}{(C_p/C_v)(R/M)T} | ||
+ | </math> | ||
+ | |||
+ | By combining this equations, we can get general relation: | ||
+ | |||
+ | \rho = \hat \rho + \frac{\partial \rho}{\partial p} \Delta p | ||
+ | |||
* 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>: |
Revision as of 20:28, 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:
Ideal gas:
By combining this equations, we can get general relation:
\rho = \hat \rho + \frac{\partial \rho}{\partial p} \Delta p
- Liquid volume transport
Let us consider transport of liquid (heavy phase) volume fraction :
By converting to volume fluxes we get:
Using equation of state, we can reformulate substantial derivative for density in terms of pressure for any phase:
* Phase change model * Momentum equation * Energy equation