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Right now we are using a first order upwind scheme for particles falling. This is very diffusive. We can do better with a second order finite volume upwind scheme.
One potential issue is that these schemes depend on the size of the timestep. We can get the size of the timestep from CVODE, in the RHS function. I just worry that this will be an issue.
The text was updated successfully, but these errors were encountered:
Right now we are using a first order upwind scheme for particles falling. This is very diffusive. We can do better with a second order finite volume upwind scheme.
See Chapter 6 in LeVeque.
One potential issue is that these schemes depend on the size of the timestep. We can get the size of the timestep from CVODE, in the RHS function. I just worry that this will be an issue.
The text was updated successfully, but these errors were encountered: