# Subgrid variance

(Difference between revisions)
 Revision as of 13:06, 15 November 2005 (view source)Salva (Talk | contribs)← Older edit Latest revision as of 11:19, 11 January 2006 (view source)Salva (Talk | contribs) m Line 7: Line 7: An equation for the subgrid variance is An equation for the subgrid variance is + :$+ \frac{\partial \overline{\rho} \widetilde{Z_{sgs}''^2} }{\partial t} + + \frac{\partial \overline{\rho} \widetilde{u}_j \widetilde{Z_{sgs}''^2} }{\partial x_j}= + \frac{\partial}{\partial x_j}\left(D \frac{\partial \widetilde{Z_{sgs}''^2} }{\partial x_j} \right) + -2 D \widetilde{\frac{\partial Z}{\partial x_j}\frac{\partial Z }{\partial x_j}} + + 2 D \frac{\partial \tilde{Z}}{\partial x_j}\frac{\partial \tilde{Z}}{\partial x_j} - + \frac{\partial J_j}{\partial x_j} + + 2 \tilde{Z} \frac{\partial}{\partial x_j} + \left( \widetilde{\rho u_j Z}- \overline{\rho}\tilde{u}_j \tilde{Z} \right) +$ + + where $J_j = \widetilde{\rho u_j {Z_{sgs}''^2}}- \overline{\rho} \tilde{u_j} \widetilde{Z_{sgs}''^2}$ is a subgrid variance flux and is often modeled using a gradient approach with turbulent diffusivity. Instead of solving the above equation, algebraic models are often used. Instead of solving the above equation, algebraic models are often used.

## Latest revision as of 11:19, 11 January 2006

The subgrid variance of a passive scalar is defined as

$\widetilde{Z_{sgs}''^2} = \widetilde{Z^2}- \widetilde{Z}^2$

The scalar subgrid variance is also known as the subgrid scalar energy in analogy to the kinetic subgrid energy. An equation for the subgrid variance is

$\frac{\partial \overline{\rho} \widetilde{Z_{sgs}''^2} }{\partial t} + \frac{\partial \overline{\rho} \widetilde{u}_j \widetilde{Z_{sgs}''^2} }{\partial x_j}= \frac{\partial}{\partial x_j}\left(D \frac{\partial \widetilde{Z_{sgs}''^2} }{\partial x_j} \right) -2 D \widetilde{\frac{\partial Z}{\partial x_j}\frac{\partial Z }{\partial x_j}} + 2 D \frac{\partial \tilde{Z}}{\partial x_j}\frac{\partial \tilde{Z}}{\partial x_j} - \frac{\partial J_j}{\partial x_j} + 2 \tilde{Z} \frac{\partial}{\partial x_j} \left( \widetilde{\rho u_j Z}- \overline{\rho}\tilde{u}_j \tilde{Z} \right)$

where $J_j = \widetilde{\rho u_j {Z_{sgs}''^2}}- \overline{\rho} \tilde{u_j} \widetilde{Z_{sgs}''^2}$ is a subgrid variance flux and is often modeled using a gradient approach with turbulent diffusivity.

Instead of solving the above equation, algebraic models are often used. For dimensional analysis

$\widetilde{Z_{sgs}''^2} = C_Z \Delta^2 \frac{\partial \widetilde{Z} }{\partial x_i} \frac{\partial \widetilde{Z} }{\partial x_i}$

where $C_Z$ can be obtained from the scalar spectra and its value is 0.1-0.2.