Changes between Version 333 and Version 334 of doc/app/initialization_parameters


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Timestamp:
Jun 7, 2017 3:15:19 PM (8 years ago)
Author:
sward
Comment:

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  • doc/app/initialization_parameters

    v333 v334  
    773773{{{#!td
    774774Switch to steer the call of the pressure solver.\\\\
    775 In order to speed-up performance, the Poisson equation for perturbation pressure (see [#psolver psolver]) can be called only at the last substep of multistep Runge-Kutta time step schemes (see [#timestep_scheme timestep_scheme]) by setting '''call_psolver_at_all_substeps''' = ''.F.''. In many cases, this sufficiently reduces the divergence of the velocity field. Nevertheless, small-scale ripples (2-delta-x) may occur. In this case and in case of non-cyclic lateral boundary conditions, the default value '''call_psolver_at_all_substeps''' = ''.T.'' should be used.
     775In order to speed-up performance, the Poisson equation for perturbation pressure (see [#psolver psolver]) can be called only at the last substep of multistep Runge-Kutta time step schemes (see [#timestep_scheme timestep_scheme]) by setting '''call_psolver_at_all_substeps''' = ''.F.''. In many cases, this sufficiently reduces the divergence of the velocity field. Nevertheless, small-scale ripples (2-delta-x) may occur. In this case and in case of non-cyclic lateral boundary conditions, the default value '''call_psolver_at_all_substeps''' = ''.T.'' should be used.\\\\
     776Pressure solver must be called at each RK3 substep when [#momentum_advec momentum_advec] = 'ws-scheme'.
    776777}}}
    777778|----------------