# SST k-omega model

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:<math> | :<math> | ||

- | \ | + | \phi = \phi_1 F_1 + \phi_2 (1 - F_1) |

</math> | </math> | ||

:<math> | :<math> | ||

- | \beta_1 = {{3} \over {40}} \beta_2 = 0.0828 | + | \alpha_1 = {{5} \over {9}}, \alpha_2 = 0.44 |

+ | </math> | ||

+ | |||

+ | :<math> | ||

+ | \beta_1 = {{3} \over {40}}, \beta_2 = 0.0828 | ||

</math> | </math> | ||

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:<math> | :<math> | ||

- | \sigma_{k1} = 0.85 \sigma_{k2} = 1 | + | \sigma_{k1} = 0.85, \sigma_{k2} = 1 |

</math> | </math> | ||

:<math> | :<math> | ||

- | \sigma_{\omega 1} = 0.5 \sigma_{\omega 2} = 0.856 | + | \sigma_{\omega 1} = 0.5, \sigma_{\omega 2} = 0.856 |

</math> | </math> | ||

## Revision as of 08:16, 11 October 2005

## Contents |

## Kinematic Eddy Viscosity

## Turbulence Kinetic Energy

## Specific Dissipation Rate

## Closure Coefficients and Auxilary Relations

## References

**Wilcox, D.C. (1988)**, "Re-assessment of the scale-determining equation for advanced turbulence models", AIAA Journal, vol. 31, pp. 1414-1421.