SST k-omega model
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- | F_1=\mbox{tanh} \left{ \left{ \mbox{min} \left[ \mbox{max} \left( {\sqrt{k} \over \beta^*\omega y}, | + | F_1=\mbox{tanh} \left{ \left{ \mbox{min} \left[ \mbox{max} \left( {\sqrt{k} \over \beta^*\omega y}, |
</math> | </math> | ||
+ | :<math> | ||
+ | {500 \nu \over y^2 \omega } \right) , {4 \sigma_{\omega 2} k} \over CD_{k\omega} y^2} \right] \right}^4 \right} | ||
+ | </math> | ||
:<math> | :<math> |
Revision as of 07:23, 11 October 2005
Contents |
Kinematic Eddy Viscosity
Turbulence Kinetic Energy
Specific Dissipation Rate
Closure Coefficients and Auxilary Relations
- Failed to parse (syntax error): F_1=\mbox{tanh} \left{ \left{ \mbox{min} \left[ \mbox{max} \left( {\sqrt{k} \over \beta^*\omega y},
- Failed to parse (syntax error): {500 \nu \over y^2 \omega } \right) , {4 \sigma_{\omega 2} k} \over CD_{k\omega} y^2} \right] \right}^4 \right}
References
- Wilcox, D.C. (1988), "Re-assessment of the scale-determining equation for advanced turbulence models", AIAA Journal, vol. 31, pp. 1414-1421.