Changes between Version 162 and Version 163 of FluxLimitedDiffusion
- Timestamp:
- 04/03/13 11:32:45 (12 years ago)
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FluxLimitedDiffusion
v162 v163 58 58 although the RHS is now more difficult to evaluate as 59 59 60 [[latex( f \left ( \tau_\nu \right ) = f \left ( s \left ( \tau_nu \right ) \right ) = f \left ( \mathbf{x} \left (s \left ( \tau_nu \right ) \right ), t \left ( s \left ( \tau_nu \right ) \right ) \right ) )]] 60 [[latex( f \left ( \tau_\nu \right ) = f \left ( s \left ( \tau_\nu \right ) \right ) = f \left ( \mathbf{x} \left (s \left ( \tau_\nu \right ) \right ), t \left ( s \left ( \tau_\nu \right ) \right ) \right ) )]] 61 62 Also if we include scattering then the source function can depend on the mean incident flux [[latex(J)]] and the transport equation becomes an integro-differential equation that must be solved iteratively... 61 63 62 64 There are also a few important dimensionless numbers to consider:
