Interface Turbulence Damping Model Reference
At a liquid-gas interface with a high relative velocity between the phases, the large gradients in the boundary layer near the free surface can cause significant turbulence fluctuations. The Interface Turbulence Damping model accounts for this in VOF multiphase simulations. This model is available for K-Epsilon, K-Omega, and Reynolds Stress Transport Turbulence.
Example applications include the flow of water on the windows of a moving motor vehicle and annular gas-liquid flows in steam generators and oil and gas production. In these cases the liquid flow is relatively slow and dominated by surface tension, but the gas flow velocity can be large (30 - 50 m/s) and aerodynamic forces are significant.
Theory | See Interface Turbulence Damping. | ||
Provided By | |||
Example Node Path | |||
Requires |
Physics continuum selections:
A VOF-VOF Phase Interaction is required. Phase interaction selections:
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Properties | None. | ||
Specific Right-Click Actions | None. | ||
Activates | Physics Models | None. | |
Model Controls (child nodes) |
Damping Coefficient For K-Omega turbulence, the damping coefficient in Eqn. (2635). For K-Epsilon or Reynolds Stress Transport turbulence, the damping coefficient in Eqn. (2636). The default value is 500. |
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Field Functions |
Interface Turbulence Damping Coefficient,
Interface Turbulence Damping Source Term.
See Field Functions. |
Field Functions
The Interface Turbulence Damping model activates the following field functions:
- Interface Turbulence Damping Coefficient
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For K-Omega turbulence, the damping coefficient in Eqn. (2635).
For K-Epsilon or Reynolds Stress Transport turbulence, the damping coefficient in Eqn. (2636).
- Interface Turbulence Damping Source Term
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For K-Omega turbulence, the term in Eqn. (2635).
For K-Epsilon or Reynolds Stress Transport turbulence, the term in Eqn. (2636).
Available only when temporary storage is activated in the appropriate Turbulence solver.