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bc2amr.f.html |
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Source file: bc2amr.f
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Directory: /home/rjl/git/rjleveque/clawpack-4.x/amrclaw/2d/lib
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Converted: Sun May 15 2011 at 19:16:13
using clawcode2html
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This documentation file will
not reflect any later changes in the source file.
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c
c ------------------------------------------------------------------
c
subroutine bc2amr(val,aux,nrow,ncol,meqn,naux,
1 hx, hy, level, time,
2 xleft, xright, ybot, ytop,
3 xlower, ylower,xupper,yupper,
4 xperiodic, yperiodic,spheredom)
c
c
c :::::::::: bc2amr ::::::::::::::::::::::::::::::::::::::::::::::;
c
c Take a grid patch with mesh widths hx,hy, of dimensions nrow by
c ncol, and set the values of any piece of
c of the patch which extends outside the physical domain
c using the boundary conditions.
c
c ------------------------------------------------
c # Standard boundary condition choices for amr2ez in clawpack
c
c # At each boundary k = 1 (left), 2 (right), 3 (bottom), 4 (top):
c # mthbc(k) = 0 for user-supplied BC's (must be inserted!)
c # = 1 for zero-order extrapolation
c # = 2 for periodic boundary conditions
c # = 3 for solid walls, assuming this can be implemented
c # by reflecting the data about the boundary and then
c # negating the 2'nd (for k=1,2) or 3'rd (for k=3,4)
c # component of q.
c # = 4 sphere bcs (left half maps to right half of same
c # side, and vice versa), as if domain folded in half
c ------------------------------------------------
c
c The corners of the grid patch are at
c (xleft,ybot) -- lower left corner
c (xright,ytop) -- upper right corner
c
c The physical domain itself is a rectangle bounded by
c (xlower,ylower) -- lower left corner
c (xupper,yupper) -- upper right corner
c
c the picture is the following:
c
c _____________________ (xupper,yupper)
c | |
c _________ (xright,ytop) |
c | | | |
c | | | |
c | | | |
c |___|____| |
c (xleft,ybot) | |
c | |
c |_____________________|
c (xlower,ylower)
c
c
c Any cells that lie outside the physical domain are ghost cells whose
c values should be set in this routine. This is tested for by comparing
c xleft with xlower to see if values need to be set at the left, as in
c the figure above, and similarly at the other boundaries.
c
c Patches are guaranteed to have at least 1 row of cells filled
c with interior values so it is possible to extrapolate.
c Fix trimbd if you want more than 1 row pre-set.
c
c Make sure the order the boundaries are specified is correct
c so that diagonal corner cells are also properly taken care of.
c
c Periodic boundaries are set before calling this routine, so if the
c domain is periodic in one direction only you
c can safely extrapolate in the other direction.
c
c Don't overwrite ghost cells in periodic directions!
c
c ::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::;
implicit double precision (a-h,o-z)
common /combc2/ mthbc(4)
dimension val(nrow,ncol,meqn), aux(nrow,ncol,naux)
logical xperiodic, yperiodic, spheredom
hxmarg = hx*.01
hymarg = hy*.01
if (xperiodic .and. (yperiodic .or. spheredom)) go to 499
c
c
c-------------------------------------------------------
c # left boundary:
c-------------------------------------------------------
if (xleft .ge. xlower-hxmarg) then
c # not a physical boundary -- no cells at this edge lies
c # outside the physical bndry.
c # values are set elsewhere in amr code.
go to 199
endif
c
c # number of grid cells from this patch lying outside physical domain:
nxl = (xlower+hxmarg-xleft)/hx
c
go to (100,110,120,130) mthbc(1)+1
c
100 continue
c # user-specified boundary conditions go here in place of error output
write(6,*)
& '*** ERROR *** mthbc(1)=0 and no BCs specified in bc2amr'
stop
go to 199
c
110 continue
c # zero-order extrapolation:
do 115 m=1,meqn
do 115 i=1,nxl
do 115 j = 1,ncol
val(i,j,m) = val(nxl+1,j,m)
115 continue
go to 199
120 continue
c # periodic: handled elsewhere in amr
go to 199
130 continue
c # solid wall (assumes 2'nd component is velocity or momentum in x):
do 135 m=1,meqn
do 135 i=1,nxl
do 135 j = 1,ncol
val(i,j,m) = val(2*nxl+1-i,j,m)
135 continue
c # negate the normal velocity:
do 136 i=1,nxl
do 136 j = 1,ncol
val(i,j,2) = -val(i,j,2)
136 continue
go to 199
199 continue
c
c-------------------------------------------------------
c # right boundary:
c-------------------------------------------------------
if (xright .le. xupper+hxmarg) then
c # not a physical boundary -- no cells at this edge lies
c # outside the physical bndry.
c # values are set elsewhere in amr code.
go to 299
endif
c
c # number of grid cells lying outside physical domain:
nxr = (xright - xupper + hxmarg)/hx
ibeg = max0(nrow-nxr+1, 1)
c
go to (200,210,220,230) mthbc(2)+1
c
200 continue
c # user-specified boundary conditions go here in place of error output
write(6,*)
& '*** ERROR *** mthbc(2)=0 and no BCs specified in bc2amr'
stop
go to 299
210 continue
c # zero-order extrapolation:
do 215 m=1,meqn
do 215 i=ibeg,nrow
do 215 j = 1,ncol
val(i,j,m) = val(ibeg-1,j,m)
215 continue
go to 299
220 continue
c # periodic: handled elsewhere in amr
go to 299
230 continue
c # solid wall (assumes 2'nd component is velocity or momentum in x):
do 235 m=1,meqn
do 235 i=ibeg,nrow
do 235 j = 1,ncol
val(i,j,m) = val(2*ibeg-1-i,j,m)
235 continue
c # negate the normal velocity:
do 236 i=ibeg,nrow
do 236 j = 1,ncol
val(i,j,2) = -val(i,j,2)
236 continue
go to 299
299 continue
c
c-------------------------------------------------------
c # bottom boundary:
c-------------------------------------------------------
if (ybot .ge. ylower-hymarg) then
c # not a physical boundary -- no cells at this edge lies
c # outside the physical bndry.
c # values are set elsewhere in amr code.
go to 399
endif
c
c # number of grid cells lying outside physical domain:
nyb = (ylower+hymarg-ybot)/hy
c
go to (300,310,320,330) mthbc(3)+1
c
300 continue
c # user-specified boundary conditions go here in place of error output
write(6,*)
& '*** ERROR *** mthbc(3)=0 and no BCs specified in bc2amr'
stop
go to 399
c
310 continue
c # zero-order extrapolation:
do 315 m=1,meqn
do 315 j=1,nyb
do 315 i=1,nrow
val(i,j,m) = val(i,nyb+1,m)
315 continue
go to 399
320 continue
c # periodic: handled elsewhere in amr
go to 399
330 continue
c # solid wall (assumes 3'rd component is velocity or momentum in y):
do 335 m=1,meqn
do 335 j=1,nyb
do 335 i=1,nrow
val(i,j,m) = val(i,2*nyb+1-j,m)
335 continue
c # negate the normal velocity:
do 336 j=1,nyb
do 336 i=1,nrow
val(i,j,3) = -val(i,j,3)
336 continue
go to 399
399 continue
c
c-------------------------------------------------------
c # top boundary:
c-------------------------------------------------------
if (ytop .le. yupper+hymarg) then
c # not a physical boundary -- no cells at this edge lies
c # outside the physical bndry.
c # values are set elsewhere in amr code.
go to 499
endif
c
c # number of grid cells lying outside physical domain:
nyt = (ytop - yupper + hymarg)/hy
jbeg = max0(ncol-nyt+1, 1)
c
go to (400,410,420,430) mthbc(4)+1
c
400 continue
c # user-specified boundary conditions go here in place of error output
write(6,*)
& '*** ERROR *** mthbc(4)=0 and no BCs specified in bc2amr'
stop
go to 499
410 continue
c # zero-order extrapolation:
do 415 m=1,meqn
do 415 j=jbeg,ncol
do 415 i=1,nrow
val(i,j,m) = val(i,jbeg-1,m)
415 continue
go to 499
420 continue
c # periodic: handled elsewhere in amr
go to 499
430 continue
c # solid wall (assumes 3'rd component is velocity or momentum in y):
do 435 m=1,meqn
do 435 j=jbeg,ncol
do 435 i=1,nrow
val(i,j,m) = val(i,2*jbeg-1-j,m)
435 continue
c # negate the normal velocity:
do 436 j=jbeg,ncol
do 436 i=1,nrow
val(i,j,3) = -val(i,j,3)
436 continue
go to 499
499 continue
return
end