c--------------------------------------------------------------------- c--------------------------------------------------------------------- subroutine exact_rhs(step, fullname, width, depth, ngbclass) c--------------------------------------------------------------------- c--------------------------------------------------------------------- c--------------------------------------------------------------------- c compute the right hand side based on exact solution c--------------------------------------------------------------------- include 'header.h' double precision dtemp(5), xi, eta, zeta, dtpp, fac integer m, i, j, k, ip1, im1, jp1, jm1, km1, kp1, step character name*2, fullname*5, tail*2, ngbclass integer width, depth, intfac name=fullname(1:2) tail=fullname(4:5) c--------------------------------------------------------------------- c initialize c--------------------------------------------------------------------- do k= 0, grid_points(3)-1 do j = 0, grid_points(2)-1 do i = 0, grid_points(1)-1 do m = 1, 5 forcing(m,i,j,k) = 0.0d0 enddo enddo enddo enddo c--------------------------------------------------------------------- c xi-direction flux differences c--------------------------------------------------------------------- do k = 1, grid_points(3)-2 zeta = dble(k) * dnzm1 do j = 1, grid_points(2)-2 eta = dble(j) * dnym1 do i=0, grid_points(1)-1 xi = dble(i) * dnxm1 call exact_solution(xi, eta, zeta, dtemp) do m = 1, 5 ue(i,m) = dtemp(m) enddo dtpp = 1.0d0 / dtemp(1) do m = 2, 5 buf(i,m) = dtpp * dtemp(m) enddo cuf(i) = buf(i,2) * buf(i,2) buf(i,1) = cuf(i) + buf(i,3) * buf(i,3) + > buf(i,4) * buf(i,4) q(i) = 0.5d0*(buf(i,2)*ue(i,2) + buf(i,3)*ue(i,3) + > buf(i,4)*ue(i,4)) enddo do i = 1, grid_points(1)-2 im1 = i-1 ip1 = i+1 forcing(1,i,j,k) = forcing(1,i,j,k) - > tx2*( ue(ip1,2)-ue(im1,2) )+ > dx1tx1*(ue(ip1,1)-2.0d0*ue(i,1)+ue(im1,1)) forcing(2,i,j,k) = forcing(2,i,j,k) - tx2 * ( > (ue(ip1,2)*buf(ip1,2)+c2*(ue(ip1,5)-q(ip1)))- > (ue(im1,2)*buf(im1,2)+c2*(ue(im1,5)-q(im1))))+ > xxcon1*(buf(ip1,2)-2.0d0*buf(i,2)+buf(im1,2))+ > dx2tx1*( ue(ip1,2)-2.0d0* ue(i,2)+ue(im1,2)) forcing(3,i,j,k) = forcing(3,i,j,k) - tx2 * ( > ue(ip1,3)*buf(ip1,2)-ue(im1,3)*buf(im1,2))+ > xxcon2*(buf(ip1,3)-2.0d0*buf(i,3)+buf(im1,3))+ > dx3tx1*( ue(ip1,3)-2.0d0*ue(i,3) +ue(im1,3)) forcing(4,i,j,k) = forcing(4,i,j,k) - tx2*( > ue(ip1,4)*buf(ip1,2)-ue(im1,4)*buf(im1,2))+ > xxcon2*(buf(ip1,4)-2.0d0*buf(i,4)+buf(im1,4))+ > dx4tx1*( ue(ip1,4)-2.0d0* ue(i,4)+ ue(im1,4)) forcing(5,i,j,k) = forcing(5,i,j,k) - tx2*( > buf(ip1,2)*(c1*ue(ip1,5)-c2*q(ip1))- > buf(im1,2)*(c1*ue(im1,5)-c2*q(im1)))+ > 0.5d0*xxcon3*(buf(ip1,1)-2.0d0*buf(i,1)+ > buf(im1,1))+ > xxcon4*(cuf(ip1)-2.0d0*cuf(i)+cuf(im1))+ > xxcon5*(buf(ip1,5)-2.0d0*buf(i,5)+buf(im1,5))+ > dx5tx1*( ue(ip1,5)-2.0d0* ue(i,5)+ ue(im1,5)) enddo c--------------------------------------------------------------------- c Fourth-order dissipation c--------------------------------------------------------------------- do m = 1, 5 i = 1 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (5.0d0*ue(i,m) - 4.0d0*ue(i+1,m) +ue(i+2,m)) i = 2 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (-4.0d0*ue(i-1,m) + 6.0d0*ue(i,m) - > 4.0d0*ue(i+1,m) + ue(i+2,m)) enddo do m = 1, 5 do i = 3, grid_points(1)-4 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp* > (ue(i-2,m) - 4.0d0*ue(i-1,m) + > 6.0d0*ue(i,m) - 4.0d0*ue(i+1,m) + ue(i+2,m)) enddo enddo do m = 1, 5 i = grid_points(1)-3 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (ue(i-2,m) - 4.0d0*ue(i-1,m) + > 6.0d0*ue(i,m) - 4.0d0*ue(i+1,m)) i = grid_points(1)-2 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (ue(i-2,m) - 4.0d0*ue(i-1,m) + 5.0d0*ue(i,m)) enddo enddo enddo c--------------------------------------------------------------------- c eta-direction flux differences c--------------------------------------------------------------------- do k = 1, grid_points(3)-2 zeta = dble(k) * dnzm1 do i=1, grid_points(1)-2 xi = dble(i) * dnxm1 do j=0, grid_points(2)-1 eta = dble(j) * dnym1 call exact_solution(xi, eta, zeta, dtemp) do m = 1, 5 ue(j,m) = dtemp(m) enddo dtpp = 1.0d0/dtemp(1) do m = 2, 5 buf(j,m) = dtpp * dtemp(m) enddo cuf(j) = buf(j,3) * buf(j,3) buf(j,1) = cuf(j) + buf(j,2) * buf(j,2) + > buf(j,4) * buf(j,4) q(j) = 0.5d0*(buf(j,2)*ue(j,2) + buf(j,3)*ue(j,3) + > buf(j,4)*ue(j,4)) enddo do j = 1, grid_points(2)-2 jm1 = j-1 jp1 = j+1 forcing(1,i,j,k) = forcing(1,i,j,k) - > ty2*( ue(jp1,3)-ue(jm1,3) )+ > dy1ty1*(ue(jp1,1)-2.0d0*ue(j,1)+ue(jm1,1)) forcing(2,i,j,k) = forcing(2,i,j,k) - ty2*( > ue(jp1,2)*buf(jp1,3)-ue(jm1,2)*buf(jm1,3))+ > yycon2*(buf(jp1,2)-2.0d0*buf(j,2)+buf(jm1,2))+ > dy2ty1*( ue(jp1,2)-2.0* ue(j,2)+ ue(jm1,2)) forcing(3,i,j,k) = forcing(3,i,j,k) - ty2*( > (ue(jp1,3)*buf(jp1,3)+c2*(ue(jp1,5)-q(jp1)))- > (ue(jm1,3)*buf(jm1,3)+c2*(ue(jm1,5)-q(jm1))))+ > yycon1*(buf(jp1,3)-2.0d0*buf(j,3)+buf(jm1,3))+ > dy3ty1*( ue(jp1,3)-2.0d0*ue(j,3) +ue(jm1,3)) forcing(4,i,j,k) = forcing(4,i,j,k) - ty2*( > ue(jp1,4)*buf(jp1,3)-ue(jm1,4)*buf(jm1,3))+ > yycon2*(buf(jp1,4)-2.0d0*buf(j,4)+buf(jm1,4))+ > dy4ty1*( ue(jp1,4)-2.0d0*ue(j,4)+ ue(jm1,4)) forcing(5,i,j,k) = forcing(5,i,j,k) - ty2*( > buf(jp1,3)*(c1*ue(jp1,5)-c2*q(jp1))- > buf(jm1,3)*(c1*ue(jm1,5)-c2*q(jm1)))+ > 0.5d0*yycon3*(buf(jp1,1)-2.0d0*buf(j,1)+ > buf(jm1,1))+ > yycon4*(cuf(jp1)-2.0d0*cuf(j)+cuf(jm1))+ > yycon5*(buf(jp1,5)-2.0d0*buf(j,5)+buf(jm1,5))+ > dy5ty1*(ue(jp1,5)-2.0d0*ue(j,5)+ue(jm1,5)) enddo c--------------------------------------------------------------------- c Fourth-order dissipation c--------------------------------------------------------------------- do m = 1, 5 j = 1 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (5.0d0*ue(j,m) - 4.0d0*ue(j+1,m) +ue(j+2,m)) j = 2 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (-4.0d0*ue(j-1,m) + 6.0d0*ue(j,m) - > 4.0d0*ue(j+1,m) + ue(j+2,m)) enddo do m = 1, 5 do j = 3, grid_points(2)-4 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp* > (ue(j-2,m) - 4.0d0*ue(j-1,m) + > 6.0d0*ue(j,m) - 4.0d0*ue(j+1,m) + ue(j+2,m)) enddo enddo do m = 1, 5 j = grid_points(2)-3 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (ue(j-2,m) - 4.0d0*ue(j-1,m) + > 6.0d0*ue(j,m) - 4.0d0*ue(j+1,m)) j = grid_points(2)-2 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (ue(j-2,m) - 4.0d0*ue(j-1,m) + 5.0d0*ue(j,m)) enddo enddo enddo c--------------------------------------------------------------------- c zeta-direction flux differences c--------------------------------------------------------------------- do j=1, grid_points(2)-2 eta = dble(j) * dnym1 do i = 1, grid_points(1)-2 xi = dble(i) * dnxm1 do k=0, grid_points(3)-1 zeta = dble(k) * dnzm1 call exact_solution(xi, eta, zeta, dtemp) do m = 1, 5 ue(k,m) = dtemp(m) enddo dtpp = 1.0d0/dtemp(1) do m = 2, 5 buf(k,m) = dtpp * dtemp(m) enddo cuf(k) = buf(k,4) * buf(k,4) buf(k,1) = cuf(k) + buf(k,2) * buf(k,2) + > buf(k,3) * buf(k,3) q(k) = 0.5d0*(buf(k,2)*ue(k,2) + buf(k,3)*ue(k,3) + > buf(k,4)*ue(k,4)) enddo do k=1, grid_points(3)-2 km1 = k-1 kp1 = k+1 forcing(1,i,j,k) = forcing(1,i,j,k) - > tz2*( ue(kp1,4)-ue(km1,4) )+ > dz1tz1*(ue(kp1,1)-2.0d0*ue(k,1)+ue(km1,1)) forcing(2,i,j,k) = forcing(2,i,j,k) - tz2 * ( > ue(kp1,2)*buf(kp1,4)-ue(km1,2)*buf(km1,4))+ > zzcon2*(buf(kp1,2)-2.0d0*buf(k,2)+buf(km1,2))+ > dz2tz1*( ue(kp1,2)-2.0d0* ue(k,2)+ ue(km1,2)) forcing(3,i,j,k) = forcing(3,i,j,k) - tz2 * ( > ue(kp1,3)*buf(kp1,4)-ue(km1,3)*buf(km1,4))+ > zzcon2*(buf(kp1,3)-2.0d0*buf(k,3)+buf(km1,3))+ > dz3tz1*(ue(kp1,3)-2.0d0*ue(k,3)+ue(km1,3)) forcing(4,i,j,k) = forcing(4,i,j,k) - tz2 * ( > (ue(kp1,4)*buf(kp1,4)+c2*(ue(kp1,5)-q(kp1)))- > (ue(km1,4)*buf(km1,4)+c2*(ue(km1,5)-q(km1))))+ > zzcon1*(buf(kp1,4)-2.0d0*buf(k,4)+buf(km1,4))+ > dz4tz1*( ue(kp1,4)-2.0d0*ue(k,4) +ue(km1,4)) forcing(5,i,j,k) = forcing(5,i,j,k) - tz2 * ( > buf(kp1,4)*(c1*ue(kp1,5)-c2*q(kp1))- > buf(km1,4)*(c1*ue(km1,5)-c2*q(km1)))+ > 0.5d0*zzcon3*(buf(kp1,1)-2.0d0*buf(k,1) > +buf(km1,1))+ > zzcon4*(cuf(kp1)-2.0d0*cuf(k)+cuf(km1))+ > zzcon5*(buf(kp1,5)-2.0d0*buf(k,5)+buf(km1,5))+ > dz5tz1*( ue(kp1,5)-2.0d0*ue(k,5)+ ue(km1,5)) enddo c--------------------------------------------------------------------- c Fourth-order dissipation c--------------------------------------------------------------------- do m = 1, 5 k = 1 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (5.0d0*ue(k,m) - 4.0d0*ue(k+1,m) +ue(k+2,m)) k = 2 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (-4.0d0*ue(k-1,m) + 6.0d0*ue(k,m) - > 4.0d0*ue(k+1,m) + ue(k+2,m)) enddo do m = 1, 5 do k = 3, grid_points(3)-4 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp* > (ue(k-2,m) - 4.0d0*ue(k-1,m) + > 6.0d0*ue(k,m) - 4.0d0*ue(k+1,m) + ue(k+2,m)) enddo enddo do m = 1, 5 k = grid_points(3)-3 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (ue(k-2,m) - 4.0d0*ue(k-1,m) + > 6.0d0*ue(k,m) - 4.0d0*ue(k+1,m)) k = grid_points(3)-2 forcing(m,i,j,k) = forcing(m,i,j,k) - dssp * > (ue(k-2,m) - 4.0d0*ue(k-1,m) + 5.0d0*ue(k,m)) enddo enddo enddo c--------------------------------------------------------------------- c now change the sign of the forcing function, and modify in case c of rapid fire c--------------------------------------------------------------------- if (tail .ne. 'RF' .or. ngbclass .eq. 'S') then intfac = 0 else if (name .eq. 'HC') then intfac = step elseif (name .eq. 'VP' .or. name .eq. 'MB') then intfac = step/width endif endif fac = dsin(dble(intfac)) do k = 1, grid_points(3)-2 do j = 1, grid_points(2)-2 do i = 1, grid_points(1)-2 do m = 1, 5 forcing(m,i,j,k) = (-1.d0 + fac) * forcing(m,i,j,k) enddo enddo enddo enddo return end