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The cell-centered code for compressible FHD has several outstanding issues listed below. A major re-factor of the code was performed in Feb 2022 for a better prescription of the Dirichlet boundary conditions in the PR #98. In this PR, Dirichlet boundary conditions are assigned at the boundaries rather than a linear extrapolation to ghost cells for increased numerical stability. However several issues have emerged, both after the PR (post-Feb version) and before the PR (pre-Feb version)
Pre-Feb version: A binary mixture of gases at equilibrium confined between isothermal, no-slip walls exhibit incorrect density and energy variance in the boundary cells. When slip walls are used, all variances appear to be correct (see attached pdf file, and attached inputs file for testing). 0328MON_sim_res_pre-Feb_version.pdf and inputs_cell_cent_test.txt
Post-Feb version: For the similar setup as above, incorrect variances are observed for both slip and no-slip boundaries, with the results being much worse than the Pre-Feb version.
Revisit the treatment of energy fluxes at the walls. A previous PR (Fix bc compressible #37) addressed this issue by separately treating the various contributions (heat, Dufour, and viscous heating) at the walls.
The cell-centered code for compressible FHD has several outstanding issues listed below. A major re-factor of the code was performed in Feb 2022 for a better prescription of the Dirichlet boundary conditions in the PR #98. In this PR, Dirichlet boundary conditions are assigned at the boundaries rather than a linear extrapolation to ghost cells for increased numerical stability. However several issues have emerged, both after the PR (post-Feb version) and before the PR (pre-Feb version)