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4.9.5 Effects of Buoyancy on Turbulence

The production terms due to buoyancy are modeled as


 G_{ij} = (\overline{J_{i}U_{j}} + \overline{J_{j}U_{i}}) = - \beta(g_{i}\overline{u_{j}\theta} + g_{j}\overline{U_{i}\theta}) (4.9-24)


 \overline{U_{i}\theta} = \frac{\mu_{t}}{\rm Pr_{t}}(\frac{\partial T}{\partial X_{i}}) (4.9-25)

where Pr $_t$ is the turbulent Prandtl number for energy, with a default value of 0.85.

Using the definition of the coefficient of thermal expansion, $\beta$, given by Equation  4.4-24, the following expression is obtained for $G_{ij}$ for ideal gases:


 G_{ij} = - \frac{\mu_t}{\rho {\rm Pr}_t} \left(g_i \frac{\p... ...\partial x_j} + g_j \frac{\partial \rho}{\partial x_i} \right) (4.9-26)

figure   

Note that the buoyancy effects are not included if low-Re omega based RSM model is used.


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