Module with finite volume methods for fluxes. More...
Functions/Subroutines | |
| subroutine, public | hancock (qdt, dtfactor, ixIL, ixOL, idimsLIM, qtC, sCT, qt, snew, dxs, x) |
| The non-conservative Hancock predictor for TVDLF. More... | |
| subroutine, public | finite_volume (method, qdt, dtfactor, ixIL, ixOL, idimsLIM, qtC, sCT, qt, snew, fC, fE, dxs, x) |
| finite volume method More... | |
| subroutine, public | reconstruct_lr (ixIL, ixLL, ixRL, idims, w, wLC, wRC, wLp, wRp, x, dxdim) |
| Determine the upwinded wLC(ixL) and wRC(ixR) from w. the wCT is only used when PPM is exploited. More... | |
Detailed Description
Module with finite volume methods for fluxes.
Function/Subroutine Documentation
◆ finite_volume()
| subroutine, public mod_finite_volume::finite_volume | ( | integer, intent(in) | method, |
| double precision, intent(in) | qdt, | ||
| double precision, intent(in) | dtfactor, | ||
| integer, intent(in) | ixI, | ||
| integer, intent(in) | L, | ||
| integer, intent(in) | ixO, | ||
| L, | |||
| integer, intent(in) | idims, | ||
| integer, intent(in) | LIM, | ||
| double precision, intent(in) | qtC, | ||
| type(state) | sCT, | ||
| double precision, intent(in) | qt, | ||
| type(state) | snew, | ||
| double precision, dimension(ixi^s,1:nwflux,1:ndim) | fC, | ||
| double precision, dimension(ixi^s,sdim:3) | fE, | ||
| double precision, dimension(ndim), intent(in) | dxs, | ||
| double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
| ) |
finite volume method
Definition at line 116 of file mod_finite_volume.t.
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◆ hancock()
| subroutine, public mod_finite_volume::hancock | ( | double precision, intent(in) | qdt, |
| double precision, intent(in) | dtfactor, | ||
| integer, intent(in) | ixI, | ||
| integer, intent(in) | L, | ||
| integer, intent(in) | ixO, | ||
| L, | |||
| integer, intent(in) | idims, | ||
| integer, intent(in) | LIM, | ||
| double precision, intent(in) | qtC, | ||
| type(state) | sCT, | ||
| double precision, intent(in) | qt, | ||
| type(state) | snew, | ||
| double precision, dimension(ndim), intent(in) | dxs, | ||
| double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
| ) |
The non-conservative Hancock predictor for TVDLF.
on entry: input available on ixI^L=ixG^L asks for output on ixO^L=ixG^L^LSUBnghostcells one entry: (predictor): wCT – w_n wnew – w_n qdt=dt/2 on exit : (predictor): wCT – w_n wnew – w_n+1/2
Definition at line 19 of file mod_finite_volume.t.
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◆ reconstruct_lr()
| subroutine, public mod_finite_volume::reconstruct_lr | ( | integer, intent(in) | ixI, |
| integer, intent(in) | L, | ||
| integer, intent(in) | ixL, | ||
| L, | |||
| integer, intent(in) | ixR, | ||
| L, | |||
| integer, intent(in) | idims, | ||
| double precision, dimension(ixi^s,1:nw) | w, | ||
| double precision, dimension(ixi^s,1:nw) | wLC, | ||
| double precision, dimension(ixi^s,1:nw) | wRC, | ||
| double precision, dimension(ixi^s,1:nw) | wLp, | ||
| double precision, dimension(ixi^s,1:nw) | wRp, | ||
| double precision, dimension(ixi^s,1:ndim) | x, | ||
| double precision, intent(in) | dxdim | ||
| ) |
Determine the upwinded wLC(ixL) and wRC(ixR) from w. the wCT is only used when PPM is exploited.
Definition at line 1134 of file mod_finite_volume.t.
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