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edhill |
1.2 |
C $Header: /u/gcmpack/MITgcm/pkg/flt/flt_bilinear.F,v 1.1 2001/09/13 17:43:55 adcroft Exp $ |
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C $Name: $ |
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adcroft |
1.1 |
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#include "FLT_CPPOPTIONS.h" |
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subroutine flt_bilinear( |
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I xp, |
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I yp, |
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O uu, |
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I kp, |
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I u, |
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I nu, |
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I bi, |
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I bj |
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& ) |
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c ================================================================== |
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c SUBROUTINE flt_bilinear |
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c ================================================================== |
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c |
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c o Bilinear scheme to find u of particle at given xp,yp location |
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c |
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c ================================================================== |
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c SUBROUTINE flt_bilinear |
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c ================================================================== |
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c == global variables == |
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#include "SIZE.h" |
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c == routine arguments == |
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_RL xp, yp |
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_RL uu |
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integer nu, kp, bi, bj |
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_RL u (1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr,nSx,nSy) |
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c == local variables == |
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INTEGER nnx, nny, nfx, nfy, nfxp, nfyp |
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_RL dx, dy, ddx, ddy |
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integer ip |
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_RL xx, yy, phi, scalex, scaley |
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_RL u11, u12, u22, u21 |
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c == end of interface == |
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nnx = int(xp) |
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nny = int(yp) |
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dx = xp - float(nnx) |
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dy = yp - float(nny) |
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c |
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edhill |
1.2 |
c to choose the u box in which the particle is found |
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adcroft |
1.1 |
c nu=1 for T, S |
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c nu=2 for u |
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c nu=3 for v |
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c nu=4 for w |
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c |
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if (nu.eq.1.or.nu.eq.4) then |
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nfx = nnx |
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nfy = nny |
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ddx = dx |
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ddy = dy |
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endif |
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c |
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if (nu.eq.2) then |
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if (dx.le.0.5) then |
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nfx = nnx |
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ddx = dx + 0.5 |
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else |
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nfx = nnx + 1 |
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ddx = dx - 0.5 |
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endif |
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nfy = nny |
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ddy = dy |
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endif |
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c |
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if (nu.eq.3) then |
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if (dy.le.0.5) then |
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nfy = nny |
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ddy = dy + 0.5 |
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else |
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nfy = nny + 1 |
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ddy = dy - 0.5 |
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endif |
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nfx = nnx |
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ddx = dx |
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endif |
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c |
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c |
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cab change start |
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c was correct only for global? |
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c if(nfx.gt.nx) nfx=nfx-nx |
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if(nfx.gt.nx) nfx=nx |
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cab change end |
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if(nfy.gt.ny) nfy=ny |
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nfxp = nfx + 1 |
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nfyp = nfy + 1 |
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cab change start |
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c if (nfx.eq.nx) nfxp = 1 |
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if (nfx.eq.nx) nfxp = nfx |
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cab change end |
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if (nfy.eq.ny) nfyp = nfy |
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if (nu.lt.4) then |
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u11 = u(nfx,nfy,kp,bi,bj) |
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u21 = u(nfxp,nfy,kp,bi,bj) |
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u22 = u(nfxp,nfyp,kp,bi,bj) |
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u12 = u(nfx,nfyp,kp,bi,bj) |
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endif |
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if (nu.eq.4) then |
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edhill |
1.2 |
caw This may be incorrect. |
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adcroft |
1.1 |
u11 = u(nfx,nfy,kp,bi,bj)+u(nfx,nfy,kp-1,bi,bj) |
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u21 = u(nfxp,nfy,kp,bi,bj)+u(nfxp,nfy,kp-1,bi,bj) |
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u22 = u(nfxp,nfyp,kp,bi,bj)+u(nfxp,nfyp,kp-1,bi,bj) |
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u12 = u(nfx,nfyp,kp,bi,bj)+u(nfx,nfyp,kp-1,bi,bj) |
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endif |
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edhill |
1.2 |
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adcroft |
1.1 |
c |
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c |
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c bilinear interpolation (from numerical recipes) |
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uu = (1-ddx)*(1-ddy)*u11 + ddx*(1-ddy)*u21 + ddx*ddy*u22 |
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. + (1-ddx)*ddy*u12 |
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c |
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c |
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return |
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end |
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edhill |
1.2 |
subroutine flt_trilinear( |
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I xp, |
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I yp, |
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I zp, |
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O uu, |
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I u, |
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I nu, |
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I bi, |
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I bj |
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& ) |
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c ================================================================== |
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c SUBROUTINE flt_trilinear |
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c ================================================================== |
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c |
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c o Trilinear scheme to find u of particle at a given xp,yp,zp |
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c location. This routine is a straight forward generalization of the |
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c bilinear interpolation scheme. |
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c |
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c started: 2004.05.28 Antti Westerlund (antti.westerlund@fimr.fi) |
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c and Sergio Jaramillo (sju@eos.ubc.ca). |
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c (adopted from subroutine bilinear by Arne Biastoch) |
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c |
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c ================================================================== |
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c SUBROUTINE flt_trilinear |
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c ================================================================== |
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c == global variables == |
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#include "SIZE.h" |
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c == routine arguments == |
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_RL xp, yp, zp |
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_RL uu |
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integer nu, bi, bj |
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_RL u (1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr,nSx,nSy) |
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c == local variables == |
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INTEGER nnx, nny, nnz, nfx, nfy, nfz, nfxp, nfyp, nfzp |
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_RL dx, dy, dz, ddx, ddy, ddz |
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integer ip |
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_RL xx, yy, zz, phi, scalex, scaley, scalez |
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_RL u111, u121, u221, u211, u112, u122, u222, u212 |
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c == end of interface == |
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c Round xp,yp,zp down to find a grid point. |
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nnx = int(xp) |
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nny = int(yp) |
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nnz = int(zp) |
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c Find out the distance from the gridpoint. |
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dx = xp - float(nnx) |
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dy = yp - float(nny) |
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dz = zp - float(nnz) |
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c |
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c to choose the u box in which the particle is found |
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c nu=1 for T, S |
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c nu=2 for u |
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c nu=3 for v |
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c nu=4 for w |
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c |
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c Velocities are face quantities and must therefore be treated differently |
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c |
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c if the variable is T,S |
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if (nu.eq.1) then |
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nfx = nnx |
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ddx = dx |
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nfy = nny |
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ddy = dy |
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nfz = nnz |
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ddz = dz |
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endif |
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c if the variable is u |
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if (nu.eq.2) then |
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if (dx.le.0.5) then |
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nfx = nnx |
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ddx = dx + 0.5 |
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else |
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nfx = nnx + 1 |
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ddx = dx - 0.5 |
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endif |
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nfy = nny |
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ddy = dy |
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nfz = nnz |
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ddz = dz |
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endif |
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c if the variable is v |
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if (nu.eq.3) then |
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nfx = nnx |
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ddx = dx |
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if (dy.le.0.5) then |
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nfy = nny |
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ddy = dy + 0.5 |
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else |
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nfy = nny + 1 |
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ddy = dy - 0.5 |
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endif |
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nfz = nnz |
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ddz = dz |
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endif |
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c if the variable is w |
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if (nu.eq.4) then |
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nfx = nnx |
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ddx = dx |
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nfy = nny |
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ddy = dy |
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if (dz.le.0.5) then |
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nfz = nnz |
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ddz = dz + 0.5 |
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else |
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nfz = nnz + 1 |
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ddz = dz - 0.5 |
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endif |
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endif |
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c |
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c if we are near or over the edge, limit nfx/y/z |
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if(nfx.gt.nx) nfx=nx |
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if(nfy.gt.ny) nfy=ny |
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if(nfz.gt.nr) nfz=nr |
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if(nfz.le.1) nfz=1 |
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c We should possibly check something else too... |
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c |
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c the coordinates for the other grid points |
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nfxp = nfx + 1 |
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nfyp = nfy + 1 |
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nfzp = nfz + 1 |
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c if we are near the edge, also limit nf?p |
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if (nfx.eq.nx) nfxp = nfx |
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if (nfy.eq.ny) nfyp = nfy |
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if (nfz.eq.nr) nfzp = nfz |
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c Values of the field at relevant grid points |
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u111 = u(nfx,nfy,nfz,bi,bj) |
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u211 = u(nfxp,nfy,nfz,bi,bj) |
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u221 = u(nfxp,nfyp,nfz,bi,bj) |
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u121 = u(nfx,nfyp,nfz,bi,bj) |
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u112 = u(nfx,nfy,nfzp,bi,bj) |
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u212 = u(nfxp,nfy,nfzp,bi,bj) |
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u222 = u(nfxp,nfyp,nfzp,bi,bj) |
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u122 = u(nfx,nfyp,nfzp,bi,bj) |
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c Trilinear interpolation, a straight forward generalization |
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c of the bilinear interpolation scheme. |
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uu = (1-ddx)*(1-ddy)*(1-ddz)*u111 + ddx*(1-ddy)*(1-ddz)*u211 |
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& + ddx*ddy*(1-ddz)*u221 + (1-ddx)*ddy*(1-ddz)*u121 |
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& + (1-ddx)*(1-ddy)*ddz*u112 + ddx*(1-ddy)*ddz*u212 |
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& + ddx*ddy*ddz*u222 + (1-ddx)*ddy*ddz*u122 |
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c |
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c |
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return |
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end |
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adcroft |
1.1 |
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subroutine flt_bilinear2d( |
| 285 |
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I xp, |
| 286 |
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I yp, |
| 287 |
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O uu, |
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I u, |
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I nu, |
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I bi, |
| 291 |
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I bj |
| 292 |
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& ) |
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c ================================================================== |
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c SUBROUTINE flt_bilinear2d |
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c ================================================================== |
| 297 |
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c |
| 298 |
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c o Bilinear scheme to find u of particle at given xp,yp location |
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c o For 2D fields |
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c |
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c started: Arne Biastoch abiastoch@ucsd.edu 13-Jan-2000 |
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c (adopted from subroutine bilinear) |
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c |
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c ================================================================== |
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c SUBROUTINE flt_bilinear2d |
| 306 |
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c ================================================================== |
| 307 |
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| 308 |
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c == global variables == |
| 309 |
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| 310 |
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#include "SIZE.h" |
| 311 |
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| 312 |
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c == routine arguments == |
| 313 |
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| 314 |
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_RL xp, yp |
| 315 |
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_RL uu |
| 316 |
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integer nu, bi, bj |
| 317 |
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_RL u (1-OLx:sNx+OLx,1-OLy:sNy+OLy,nSx,nSy) |
| 318 |
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| 319 |
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c == local variables == |
| 320 |
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| 321 |
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INTEGER nnx, nny, nfx, nfy, nfxp, nfyp |
| 322 |
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_RL dx, dy, ddx, ddy |
| 323 |
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integer ip |
| 324 |
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_RL xx, yy, phi, scalex, scaley |
| 325 |
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_RL u11, u12, u22, u21 |
| 326 |
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| 327 |
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c == end of interface == |
| 328 |
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| 329 |
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nnx = int(xp) |
| 330 |
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nny = int(yp) |
| 331 |
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dx = xp - float(nnx) |
| 332 |
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dy = yp - float(nny) |
| 333 |
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c |
| 334 |
edhill |
1.2 |
c to choose the u box in which the particle is found |
| 335 |
adcroft |
1.1 |
c nu=1 for T, S |
| 336 |
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c nu=2 for u |
| 337 |
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c nu=3 for v |
| 338 |
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c nu=4 for w |
| 339 |
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c |
| 340 |
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if (nu.eq.1.or.nu.eq.4) then |
| 341 |
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nfx = nnx |
| 342 |
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nfy = nny |
| 343 |
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ddx = dx |
| 344 |
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ddy = dy |
| 345 |
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endif |
| 346 |
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c |
| 347 |
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if (nu.eq.2) then |
| 348 |
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if (dx.le.0.5) then |
| 349 |
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nfx = nnx |
| 350 |
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ddx = dx + 0.5 |
| 351 |
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else |
| 352 |
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nfx = nnx + 1 |
| 353 |
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ddx = dx - 0.5 |
| 354 |
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endif |
| 355 |
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nfy = nny |
| 356 |
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ddy = dy |
| 357 |
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endif |
| 358 |
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c |
| 359 |
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if (nu.eq.3) then |
| 360 |
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if (dy.le.0.5) then |
| 361 |
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nfy = nny |
| 362 |
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ddy = dy + 0.5 |
| 363 |
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else |
| 364 |
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nfy = nny + 1 |
| 365 |
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ddy = dy - 0.5 |
| 366 |
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endif |
| 367 |
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nfx = nnx |
| 368 |
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ddx = dx |
| 369 |
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endif |
| 370 |
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c |
| 371 |
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cab change start |
| 372 |
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c was correct only for global? |
| 373 |
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c if(nfx.gt.nx) nfx=nfx-nx |
| 374 |
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if(nfx.gt.nx) nfx=nx |
| 375 |
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cab change end |
| 376 |
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if(nfy.gt.ny) nfy=ny |
| 377 |
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nfxp = nfx + 1 |
| 378 |
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nfyp = nfy + 1 |
| 379 |
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cab change start |
| 380 |
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c if (nfx.eq.nx) nfxp = 1 |
| 381 |
|
|
if (nfx.eq.nx) nfxp = nfx |
| 382 |
|
|
cab change end |
| 383 |
|
|
if (nfy.eq.ny) nfyp = nfy |
| 384 |
|
|
|
| 385 |
|
|
if (nu.lt.4) then |
| 386 |
|
|
u11 = u(nfx,nfy,bi,bj) |
| 387 |
|
|
u21 = u(nfxp,nfy,bi,bj) |
| 388 |
|
|
u22 = u(nfxp,nfyp,bi,bj) |
| 389 |
|
|
u12 = u(nfx,nfyp,bi,bj) |
| 390 |
|
|
endif |
| 391 |
|
|
if (nu.eq.4) then |
| 392 |
edhill |
1.2 |
caw This may be incorrect. |
| 393 |
adcroft |
1.1 |
u11 = u(nfx,nfy,bi,bj)+u(nfx,nfy,bi,bj) |
| 394 |
|
|
u21 = u(nfxp,nfy,bi,bj)+u(nfxp,nfy,bi,bj) |
| 395 |
|
|
u22 = u(nfxp,nfyp,bi,bj)+u(nfxp,nfyp,bi,bj) |
| 396 |
|
|
u12 = u(nfx,nfyp,bi,bj)+u(nfx,nfyp,bi,bj) |
| 397 |
|
|
endif |
| 398 |
|
|
c |
| 399 |
|
|
c |
| 400 |
|
|
c bilinear interpolation (from numerical recipes) |
| 401 |
|
|
uu = (1-ddx)*(1-ddy)*u11 + ddx*(1-ddy)*u21 + ddx*ddy*u22 |
| 402 |
|
|
. + (1-ddx)*ddy*u12 |
| 403 |
|
|
c |
| 404 |
|
|
c |
| 405 |
|
|
return |
| 406 |
|
|
end |
| 407 |
|
|
|
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