Boussinesq eddy viscosity assumption

From CFD-Wiki

Revision as of 21:30, 9 May 2006 by Jola (Talk | contribs)

(diff) ← Older revision | Latest revision (diff) | Newer revision → (diff)

In 1877 Boussinesq postulated that the momentum transfer caused by turbulent eddies can be modeled with an eddy viscosity. This is in analogy with how the momentum transfer caused by the molecular motion in a gas can be described by a molecular viscosity. The Boussinesq assumption states that the Reynolds stress tensor, $\tau_{ij}$ , is proportional to the mean strain rate tensor, $S_{ij}$ , and can be written in the following way:

$\tau_{ij} = 2 \, \mu_t \, S_{ij}$

Where $\mu_t$ is a scalar property called the eddy viscosity. The same equation can be written more explicitly as:

$-\overline{\rho u'_i u'_j} = \mu_t \, \left( \frac{\partial U_i}{\partial x_j} + \frac{\partial U_j}{\partial x_i} \right)$

The Boussinesq eddy viscosity assumption is also often called the Boussinesq hypothesis or the Boussinesq approximation.

References

Boussinesq, J. (1877), "Théorie de l’Écoulement Tourbillant", Mem. Présentés par Divers Savants Acad. Sci. Inst. Fr., Vol. 23, pp. 46-50.

This article is a stub, a short article which needs to be improved. You can help by expanding it.

Boussinesq eddy viscosity assumption

From CFD-Wiki

References

Views

My wiki

wiki navigation

wiki search

wiki toolbox