Difference between revisions of "User talk:Ferrandm"
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-\dfrac{\partial}{\partial{x_{i}}}({\rho}{\sum}_{k=1}^{N}h_{s,k}Y_{k}V_{k,i}) | -\dfrac{\partial}{\partial{x_{i}}}({\rho}{\sum}_{k=1}^{N}h_{s,k}Y_{k}V_{k,i}) | ||
+\dfrac{\partial{\sigma_{ij}}u_{i}}{\partial{x_{j}}}</math> | +\dfrac{\partial{\sigma_{ij}}u_{i}}{\partial{x_{j}}}</math> | ||
| − | + | +\dot{Q}+{\rho}{\sum}_{k-1}^{N}Y_{k}f_{k,i}(u_{i}+V_{k,i}) </math> | |
| − | +\dot{Q}+ | + | |
Revision as of 16:09, 6 June 2012
Hypotheses
The hypotheses to simplify the Navier-Stokes equations are :
- The energy balance according to Poinsot-Veynante is descreibed below :
+\dot{Q}+{\rho}{\sum}_{k-1}^{N}Y_{k}f_{k,i}(u_{i}+V_{k,i}) </math>
