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Merge pull request #49 from BrisaDavis/vctraffic
Added variable coefficient traffic reimann solver.
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Original file line number | Diff line number | Diff line change |
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! | ||
! | ||
! ========================================================= | ||
subroutine rp1(maxm,meqn,mwaves,mbc,mx,ql,qr,auxl,auxr, & | ||
fwave,s,amdq,apdq,maux) | ||
! ========================================================= | ||
! | ||
! # solve Riemann problems for the traffic equation. | ||
! # with variable speed limit umax stored in aux(i,1) | ||
! | ||
! # returns fwave's instead of waves | ||
! | ||
! # On input, ql contains the state vector at the left edge of each cell | ||
! # qr contains the state vector at the right edge of each cell | ||
! # On output, wave contains the waves, | ||
! # s the speeds, | ||
! # amdq the left-going flux difference A^- \Delta q | ||
! # apdq the right-going flux difference A^+ \Delta q | ||
! | ||
! # Note that the i'th Riemann problem has left state qr(:,i-1) | ||
! # and right state ql(:,i) | ||
! # From the basic clawpack routine step1, rp is called with ql = qr = q. | ||
! | ||
! | ||
implicit double precision (a-h,o-z) | ||
dimension ql(meqn,1-mbc:mx+mbc) | ||
dimension qr(meqn,1-mbc:mx+mbc) | ||
dimension s(mwaves,1-mbc:mx+mbc) | ||
dimension fwave(meqn,mwaves,1-mbc:mx+mbc) | ||
dimension amdq(meqn,1-mbc:mx+mbc) | ||
dimension apdq(meqn,1-mbc:mx+mbc) | ||
dimension auxl(maux,1-mbc:mx+mbc) | ||
dimension auxr(maux,1-mbc:mx+mbc) | ||
common /comlxf/ alxf | ||
! | ||
! | ||
! | ||
do 30 i=2-mbc,mx+mbc | ||
! | ||
! # Compute the fwave and speed, and fluctuations | ||
! | ||
! # compute flux in each cell and flux difference: | ||
fim1 = auxl(1,i-1)*qr(1,i-1)*(1.d0 - qr(1,i-1)) | ||
fi = auxl(1,i)*ql(1,i)*(1.d0 - ql(1,i)) | ||
fwave(1,1,i) = fi - fim1 | ||
|
||
! # compute characteristic speed in each cell: | ||
sim1 = auxl(1,i-1)*(1.d0 - 2.d0*ql(1,i-1)) | ||
si = auxl(1,i)*(1.d0 - 2.d0*ql(1,i)) | ||
|
||
if (sim1 .lt. 0.d0 .and. si .le. 0.d0) then | ||
! # left-going | ||
s(1,i) = sim1 | ||
amdq(1,i) = fwave(1,1,i) | ||
apdq(1,i) = 0.d0 | ||
else if (sim1 .ge. 0.d0 .and. si .gt. 0.d0) then | ||
! # right-going | ||
s(1,i) = si | ||
amdq(1,i) = 0.d0 | ||
apdq(1,i) = fwave(1,1,i) | ||
else if (sim1 .lt. 0.d0 .and. si .gt. 0.d0) then | ||
! # transonic rarefaction | ||
! # split fwave between amdq and apdq: | ||
s(1,i) = 0.5d0*(sim1 + si) | ||
dq = ql(1,i) - qr(1,i-1) | ||
|
||
! # entropy fix: (perhaps doesn't work for all cases!!!) | ||
! # This assumes the flux in the transonic case should | ||
! # correspond to q=0.5 on the side with the smaller umax value. | ||
f0 = dmin1(auxl(1,i-1),auxl(1,i))*0.25d0 | ||
amdq(1,i) = f0 - fim1 | ||
apdq(1,i) = fi - f0 | ||
|
||
else | ||
! # transonic shock | ||
s(1,i) = 0.5d0*(sim1 + si) | ||
if (s(1,i) .lt. 0.d0) then | ||
amdq(1,i) = fwave(1,1,i) | ||
apdq(1,i) = 0.d0 | ||
else if (s(1,i) .gt. 0.d0) then | ||
amdq(1,i) = 0.d0 | ||
apdq(1,i) = fwave(1,1,i) | ||
else | ||
amdq(1,i) = 0.5d0 * fwave(1,1,i) | ||
apdq(1,i) = 0.5d0 * fwave(1,1,i) | ||
endif | ||
endif | ||
! | ||
30 continue | ||
! | ||
return | ||
end | ||
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