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Source file: bc2quad.f | |
Directory: /home/rjl/git/rjleveque/clawpack-4.x/book/chap23/acoustics | |
Converted: Tue Jul 26 2011 at 12:58:58 using clawcode2html | |
This documentation file will not reflect any later changes in the source file. |
c c c ===================================================== subroutine bc2(maxmx,maxmy,meqn,mbc,mx,my,xlower,ylower, & dx,dy,q,maux,aux,t,dt,mthbc) c ===================================================== c c # Standard boundary condition choices for claw2, c c # Modified for a general quadrilateral grid in the case mthbc(k)=3: c # Solid wall boundary conditions are implemented by negating the c # velocity normal to the wall. c c # At each boundary k = 1 (left), 2 (right), 3 (top), 4 (bottom): c # mthbc(k) = 0 for user-supplied BC's (must be inserted!) c # = 1 for zero-order extrapolation c # = 2 for periodic boundary coniditions c # = 3 for solid walls, assuming this can be implemented c # by reflecting the data about the boundary and then c # negating the normal component of the velocity. c # On a quadrilateral grid we know the normal to each c # edge and assume this is stored in the aux array: c c # aux(i,j,1) = ax c # aux(i,j,2) = ay where (ax,ay) is unit normal to left face c # aux(i,j,4) = bx c # aux(i,j,5) = by where (bx,by) is unit normal to bottom face c ------------------------------------------------ c c # Extend the data from the interior cells (1:mx, 1:my) c # to the ghost cells outside the region: c # (i, 1-jbc) for jbc = 1,mbc, i = 1-mbc, mx+mbc c # (i, my+jbc) for jbc = 1,mbc, i = 1-mbc, mx+mbc c # (1-ibc, j) for ibc = 1,mbc, j = 1-mbc, my+mbc c # (mx+ibc, j) for ibc = 1,mbc, j = 1-mbc, my+mbc c implicit double precision (a-h,o-z) dimension q(1-mbc:maxmx+mbc, 1-mbc:maxmy+mbc, meqn) dimension aux(1-mbc:maxmx+mbc, 1-mbc:maxmy+mbc, *) dimension mthbc(4) c c c------------------------------------------------------- c # left boundary: 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 bc2' stop go to 199 c 110 continue c # zero-order extrapolation: do 115 m=1,meqn do 115 ibc=1,mbc do 115 j = 1-mbc, my+mbc q(1-ibc,j,m) = q(1,j,m) 115 continue go to 199 120 continue c # periodic: do 125 m=1,meqn do 125 ibc=1,mbc do 125 j = 1-mbc, my+mbc q(1-ibc,j,m) = q(mx+1-ibc,j,m) 125 continue go to 199 130 continue c # solid wall do 135 m=1,meqn do 135 ibc=1,mbc do 135 j = 1-mbc, my+mbc q(1-ibc,j,m) = q(ibc,j,m) 135 continue c # negate the normal velocity: c # (for a general quadrilateral grid) c do 136 ibc=1,mbc do 136 j = 1-mbc, my+mbc alf = aux(1,j,1) beta = aux(1,j,2) unorm = alf*q(ibc,j,2) + beta*q(ibc,j,3) utang = -beta*q(ibc,j,2) + alf*q(ibc,j,3) unorm = -unorm q(1-ibc,j,2) = alf*unorm - beta*utang q(1-ibc,j,3) = beta*unorm + alf*utang 136 continue go to 199 199 continue c c------------------------------------------------------- c # right boundary: 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 bc2' stop go to 299 210 continue c # zero-order extrapolation: do 215 m=1,meqn do 215 ibc=1,mbc do 215 j = 1-mbc, my+mbc q(mx+ibc,j,m) = q(mx,j,m) 215 continue go to 299 220 continue c # periodic: do 225 m=1,meqn do 225 ibc=1,mbc do 225 j = 1-mbc, my+mbc q(mx+ibc,j,m) = q(ibc,j,m) 225 continue go to 299 230 continue c # solid wall do 235 m=1,meqn do 235 ibc=1,mbc do 235 j = 1-mbc, my+mbc q(mx+ibc,j,m) = q(mx+1-ibc,j,m) 235 continue c # negate the normal velocity: c # (for a general quadrilateral grid) c do 236 ibc=1,mbc do 236 j = 1-mbc, my+mbc alf = aux(mx+1,j,1) beta = aux(mx+1,j,2) unorm = alf*q(mx+1-ibc,j,2) + beta*q(mx+1-ibc,j,3) utang = -beta*q(mx+1-ibc,j,2) + alf*q(mx+1-ibc,j,3) unorm = -unorm q(mx+ibc,j,2) = alf*unorm - beta*utang q(mx+ibc,j,3) = beta*unorm + alf*utang 236 continue go to 299 299 continue c c------------------------------------------------------- c # bottom boundary: 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 bc2' stop go to 399 c 310 continue c # zero-order extrapolation: do 315 m=1,meqn do 315 jbc=1,mbc do 315 i = 1-mbc, mx+mbc q(i,1-jbc,m) = q(i,1,m) 315 continue go to 399 320 continue c # periodic: do 325 m=1,meqn do 325 jbc=1,mbc do 325 i = 1-mbc, mx+mbc q(i,1-jbc,m) = q(i,my+1-jbc,m) 325 continue go to 399 330 continue c # solid wall do 335 m=1,meqn do 335 jbc=1,mbc do 335 i = 1-mbc, mx+mbc q(i,1-jbc,m) = q(i,jbc,m) 335 continue c # negate the normal velocity: c # (for a general quadrilateral grid) c do 336 jbc=1,mbc do 336 i = 1-mbc, mx+mbc alf = aux(i,1,4) beta = aux(i,1,5) unorm = alf*q(i,jbc,2) + beta*q(i,jbc,3) utang = -beta*q(i,jbc,2) + alf*q(i,jbc,3) unorm = -unorm q(i,1-jbc,2) = alf*unorm - beta*utang q(i,1-jbc,3) = beta*unorm + alf*utang 336 continue go to 399 399 continue c c------------------------------------------------------- c # top boundary: c------------------------------------------------------- go to (400,410,420,430) mthbc(4)+1 c 400 continue do 405 jbc=1,mbc do 405 i = 1-mbc, mx+mbc q(i,my+jbc,1) = 1.d0 405 continue go to 499 410 continue c # zero-order extrapolation: do 415 m=1,meqn do 415 jbc=1,mbc do 415 i = 1-mbc, mx+mbc q(i,my+jbc,m) = q(i,my,m) 415 continue go to 499 420 continue c # periodic: do 425 m=1,meqn do 425 jbc=1,mbc do 425 i = 1-mbc, mx+mbc q(i,my+jbc,m) = q(i,jbc,m) 425 continue go to 499 430 continue c # solid wall do 435 m=1,meqn do 435 jbc=1,mbc do 435 i = 1-mbc, mx+mbc q(i,my+jbc,m) = q(i,my+1-jbc,m) 435 continue c # negate the normal velocity: c # (for a general quadrilateral grid) c do 436 jbc=1,mbc do 436 i = 1-mbc, mx+mbc alf = aux(i,my+1,4) beta = aux(i,my+1,5) unorm = alf*q(i,my+1-jbc,2) + beta*q(i,my+1-jbc,3) utang = -beta*q(i,my+1-jbc,2) + alf*q(i,my+1-jbc,3) unorm = -unorm q(i,my+jbc,2) = alf*unorm - beta*utang q(i,my+jbc,3) = beta*unorm + alf*utang 436 continue go to 499 499 continue return end