Difference between revisions of "User talk:Bossenne"

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{{Welcome|Bossenne|Eurielle Bossennec}}
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== Motivation ==
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H-Allegro uses the compressible and reactive Navier-Stokes equations in order to solve two-phase combustion. It also takes into account a simplified chemistry of the reaction and the propagation of acoustic waves.
  
 
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* <math>
<i>H-Allegro uses the Navier-Stokes equations to solve combustion.</i>
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\dfrac{\partial{\rho}}{\partial{t}}+\dfrac{\partial{{\rho}U_{j}}}{\partial{x_{j}}}=0
 
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<math>
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(1) \dfrac{\partial{\rho}}{\partial{t}}+\dfrac{\partial{{\rho}U_{j}}}{\partial{x_{j}}}=0
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</math>
 
</math>
  
<math>
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* <math>
(2) \dfrac{\partial{{\rho}U_{i}}}{\partial{t}}+\dfrac{\partial{{\rho}}U_{i}U_{j}}{\partial{x_{j}}}+\dfrac{\partial{P}}{\partial{x_{i}}}=\dfrac{\partial{\tau_{ij}}}{\partial{x_{j}}}+S_{i}
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\dfrac{\partial{{\rho}U_{i}}}{\partial{t}}+\dfrac{\partial{{\rho}}U_{i}U_{j}}{\partial{x_{j}}}+\dfrac{\partial{P}}{\partial{x_{i}}}=\dfrac{\partial{\tau_{ij}}}{\partial{x_{j}}}+S_{i}
 
</math>
 
</math>
  
<math>
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* <math>
(3) \dfrac{\partial{{\rho}E}}{\partial{t}}+\dfrac{\partial{(P+{\rho}E)}U_{j}}{\partial{x_{j}}}=\dfrac{\partial{q_{j}}}{\partial{x_{j}}}+\dfrac{\partial{\tau_{ij}U_{i}}}{\partial{x_{j}}}+S_{5}
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\dfrac{\partial{{\rho}E}}{\partial{t}}+\dfrac{\partial{(P+{\rho}E)}U_{j}}{\partial{x_{j}}}=\dfrac{\partial{q_{j}}}{\partial{x_{j}}}+\dfrac{\partial{\tau_{ij}U_{i}}}{\partial{x_{j}}}+S_{5}
 
</math>
 
</math>
  
<math>
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* <math>
(4) \dfrac{\partial{{\rho}Y_{k}}}{\partial{t}}+\dfrac{\partial{{\rho}Y_{k}U_{j}}}{\partial{x_{j}}}=\dfrac{\partial{q_{j}^{k}}}{\partial{x_{j}}}+S_{k}
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\dfrac{\partial{{\rho}Y_{k}}}{\partial{t}}+\dfrac{\partial{{\rho}Y_{k}U_{j}}}{\partial{x_{j}}}=\dfrac{\partial{q_{j}^{k}}}{\partial{x_{j}}}+S_{k}
 
</math>
 
</math>

Revision as of 15:55, 6 June 2012

Motivation

H-Allegro uses the compressible and reactive Navier-Stokes equations in order to solve two-phase combustion. It also takes into account a simplified chemistry of the reaction and the propagation of acoustic waves.