Changes between Version 123 and Version 124 of FluxLimitedDiffusion


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Timestamp:
03/30/13 22:58:45 (12 years ago)
Author:
Jonathan
Comment:

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  • FluxLimitedDiffusion

    v123 v124  
    405405and then discretized as
    406406
    407   [[latex(e^{n+1}_i-e^{n}_i = \frac{\Delta t}{\Delta x}  \left ( f \left ( e^n_i \right ) + g \left ( e^n_i,E^*,\nabla E^* \right ) \right ) + \left ( \left ( \bar{\psi} - 1 \right ) \phi \right ) e^n_i +  \psi \phi e^{n+1}_i) ]]
    408 
    409 which can be solved for [[latex(e^{n+1} = \frac{1}{1-\psi \phi} \left ( \left ( \bar{\psi} - 1 \right ) \phi e^n_i + f \left ( e^n_i \right ) + g \left ( e^n_i,E^*,\nabla E^* \right ) \right ) )]]
     407  [[latex(e^{n+1}_i-e^{n}_i = \frac{\Delta t}{\Delta x}  \left ( f \left ( e^n_i \right ) + g \left ( e^n_i,E^*,\nabla E^* \right ) \right ) + \left ( \left ( \bar{\psi} - 1  \right ) \phi \right ) e^n_i +  \psi \phi e^{n+1}_i) ]]
     408
     409which can be solved for
     410[[latex(e^{n+1}_i = \frac{1}{1 - \psi \phi} \left ( \left ( \bar{\psi} - 1 \right ) \phi e^n_i + f \left ( e^n_i \right ) + g \left ( e^n_i,E^*,\nabla E^* \right ) \right ) )]]
    410411
    411412Then if we take the semi-discretized equation for E