stepgrid.f.html | |
Source file: stepgrid.f | |
Directory: /home/rjl/git/rjleveque/clawpack-4.x/amrclaw/2d/lib | |
Converted: Tue Jul 26 2011 at 12:59:08 using clawcode2html | |
This documentation file will not reflect any later changes in the source file. |
c c ------------------------------------------------------------- c subroutine stepgrid(q,fm,fp,gm,gp,mitot,mjtot,mbc,dt,dtnew,dx,dy, & nvar,xlow,ylow,time,mptr,maux,aux) c c c ::::::::::::::::::: STEPGRID :::::::::::::::::::::::::::::::::::: c take a time step on a single grid. overwrite solution array q. c A modified version of the clawpack routine step2 is used. c c return fluxes in fm,fp and gm,gp. c patch has room for ghost cells (mbc of them) around the grid. c everything is the enlarged size (mitot by mjtot). c c mbc = number of ghost cells (= lwidth) c mptr = grid number (for debugging) c xlow,ylow = lower left corner of enlarged grid (including ghost cells). c dt = incoming time step c dx,dy = mesh widths for this grid c dtnew = return suggested new time step for this grid's soln. c c ::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: implicit double precision (a-h,o-z) external rpn2,rpt2 include "call.i" common /comxyt/ dtcom,dxcom,dycom,tcom,icom,jcom parameter (msize=max1d+4) parameter (mwork=msize*(maxvar*maxvar + 13*maxvar + 3*maxaux +2)) dimension q(mitot,mjtot,nvar) dimension fp(mitot,mjtot,nvar),gp(mitot,mjtot,nvar) dimension fm(mitot,mjtot,nvar),gm(mitot,mjtot,nvar) dimension aux(mitot,mjtot,maux) dimension work(mwork) logical debug, dump data debug/.false./, dump/.false./ c c # set tcom = time. This is in the common block comxyt that could c # be included in the Riemann solver, for example, if t is explicitly c # needed there. tcom = time if (dump) then do i = 1, mitot do j = 1, mjtot write(outunit,545) i,j,(q(i,j,ivar),ivar=1,nvar) 545 format(2i4,4e15.7) end do end do endif c meqn = nvar mx = mitot - 2*mbc my = mjtot - 2*mbc maxm = max(mx,my) !# size for 1d scratch array mbig = maxm xlowmbc = xlow + mbc*dx ylowmbc = ylow + mbc*dy c # method(2:7) and mthlim c # are set in the amr2ez file (read by amr) c method(1) = 0 c c c # fluxes initialized in step2 c mwork0 = (maxm+2*mbc)*(12*meqn + mwaves + meqn*mwaves + 2) c if (mwork .lt. mwork0) then write(outunit,*) 'CLAW2 ERROR... mwork must be increased to ', & mwork0 write(* ,*) 'CLAW2 ERROR... mwork must be increased to ', & mwork0 stop endif c c # partition work array into pieces needed for local storage in c # step2 routine. Find starting index of each piece: c i0faddm = 1 i0faddp = i0faddm + (maxm+2*mbc)*meqn i0gaddm = i0faddp + (maxm+2*mbc)*meqn i0gaddp = i0gaddm + 2*(maxm+2*mbc)*meqn i0q1d = i0gaddp + 2*(maxm+2*mbc)*meqn i0dtdx1 = i0q1d + (maxm+2*mbc)*meqn i0dtdy1 = i0dtdx1 + (maxm+2*mbc) i0aux1 = i0dtdy1 + (maxm+2*mbc) i0aux2 = i0aux1 + (maxm+2*mbc)*maux i0aux3 = i0aux2 + (maxm+2*mbc)*maux c c i0next = i0aux3 + (maxm+2*mbc)*maux !# next free space mused = i0next - 1 !# space already used mwork1 = mwork - mused !# remaining space (passed to step2) c c call b4step2(mx,my,mbc,mx,my,nvar,q, & xlowmbc,ylowmbc,dx,dy,time,dt,maux,aux) c c c # take one step on the conservation law: c call step2(mbig,mx,my,nvar,maux, & mbc,mx,my, & q,aux,dx,dy,dt,cflgrid, & fm,fp,gm,gp, & work(i0faddm),work(i0faddp), & work(i0gaddm),work(i0gaddp), & work(i0q1d),work(i0dtdx1),work(i0dtdy1), & work(i0aux1),work(i0aux2),work(i0aux3), & work(i0next),mwork1,rpn2,rpt2) c c write(outunit,1001) mptr, node(nestlevel,mptr),cflgrid 1001 format(' Courant # of grid', i4, & ' on level', i3, ' is ', e10.3) c cflmax = dmax1(cflmax,cflgrid) cfl_level = dmax1(cfl_level,cflgrid) c c # update q dtdx = dt/dx dtdy = dt/dy do 50 m=1,nvar do 50 i=mbc+1,mitot-mbc do 50 j=mbc+1,mjtot-mbc if (mcapa.eq.0) then c c # no capa array. Standard flux differencing: q(i,j,m) = q(i,j,m) & - dtdx * (fm(i+1,j,m) - fp(i,j,m)) & - dtdy * (gm(i,j+1,m) - gp(i,j,m)) else c # with capa array. q(i,j,m) = q(i,j,m) & - (dtdx * (fm(i+1,j,m) - fp(i,j,m)) & + dtdy * (gm(i,j+1,m) - gp(i,j,m))) / aux(i,j,mcapa) endif 50 continue c c if (method(5).eq.1) then c # with source term: use Godunov splitting call src2(mx,my,nvar,mbc,mx,my,xlowmbc,ylowmbc,dx,dy, & q,maux,aux,time,dt) endif c c c c # output fluxes for debugging purposes: if (debug) then write(dbugunit,*)" fluxes for grid ",mptr do 830 i = mbc+1, mitot-1 do 830 j = mbc+1, mjtot-1 write(dbugunit,831) i,j,fm(i,j,1),fp(i,j,1), . gm(i,j,1),gp(i,j,1) do 830 m = 2, meqn write(dbugunit,832) fm(i,j,m),fp(i,j,m), . gm(i,j,m),gp(i,j,m) 831 format(2i4,4d16.6) 832 format(8x,4d16.6) 830 continue endif c c c For variable time stepping, use max speed seen on this grid to c choose the allowable new time step dtnew. This will later be c compared to values seen on other grids. c if (cflgrid .gt. 0.d0) then dtnew = dt*cfl/cflgrid else c # velocities are all zero on this grid so there's no c # time step restriction coming from this grid. dtnew = rinfinity endif c # give a warning if Courant number too large... c if (cflgrid .gt. cflv1) then write(*,810) cflgrid write(outunit,810) cflgrid, cflv1 810 format('*** WARNING *** Courant number =', d12.4, & ' is larger than input cfl_max = ', d12.4) endif c return end