rpt2ac.f.html | |
Source file: rpt2ac.f | |
Directory: /home/rjl/git/rjleveque/clawpack-4.x/doc/sphinx/example-acoustics-2d | |
Converted: Tue Jul 26 2011 at 12:46:10 using clawcode2html | |
This documentation file will not reflect any later changes in the source file. |
c c c ===================================================== subroutine rpt2(ixy,maxm,meqn,mwaves,mbc,mx, & ql,qr,aux1,aux2,aux3, & imp,asdq,bmasdq,bpasdq) c ===================================================== implicit double precision (a-h,o-z) c c # Riemann solver in the transverse direction for the acoustics equations. c c # Split asdq into down-going flux bmasdq and up-going flux bpasdq. c dimension ql(1-mbc:maxm+mbc, meqn) dimension qr(1-mbc:maxm+mbc, meqn) dimension asdq(1-mbc:maxm+mbc, meqn) dimension bmasdq(1-mbc:maxm+mbc, meqn) dimension bpasdq(1-mbc:maxm+mbc, meqn) c c # density, bulk modulus, and sound speed, and impedence of medium: c # (should be set in setprob.f) common /cparam/ rho,bulk,cc,zz c if (ixy.eq.1) then mu = 2 mv = 3 else mu = 3 mv = 2 endif c do 20 i = 2-mbc, mx+mbc a1 = (-asdq(i,1) + zz*asdq(i,mv)) / (2.d0*zz) a2 = (asdq(i,1) + zz*asdq(i,mv)) / (2.d0*zz) c c # The down-going flux difference bmasdq is the product -c * wave c bmasdq(i,1) = cc * a1*zz bmasdq(i,mu) = 0.d0 bmasdq(i,mv) = -cc * a1 c c # The up-going flux difference bpasdq is the product c * wave c bpasdq(i,1) = cc * a2*zz bpasdq(i,mu) = 0.d0 bpasdq(i,mv) = cc * a2 c 20 continue c return end