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2 changes: 1 addition & 1 deletion examples/shallow_sphere/Rossby_wave.py
Original file line number Diff line number Diff line change
Expand Up @@ -450,7 +450,7 @@ def setup(use_petsc=False,solver_type='classic',outdir='./_output', disable_outp
# Set initial conditions
# ======================
# 1) Call fortran function
qtmp = np.ndarray(shape=(solver.num_eqn,mx+2*num_ghost,my+2*num_ghost), dtype=float, order='F')
qtmp = np.zeros(shape=(solver.num_eqn,mx+2*num_ghost,my+2*num_ghost), dtype=float, order='F')
qtmp = sw_sphere_problem.qinit(mx,my,num_ghost,mx,my,xlower,ylower,dx,dy,qtmp,auxtmp,Rsphere)
state.q[:,:,:] = qtmp[:,num_ghost:-num_ghost,num_ghost:-num_ghost]

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20 changes: 11 additions & 9 deletions examples/shallow_sphere/src2.f90
Original file line number Diff line number Diff line change
@@ -1,18 +1,20 @@
! =======================================================
subroutine src2(maxmx,maxmy,num_eqn,num_ghost,mx,my,xlower,ylower, &
dx,dy,q,num_aux,aux,t,dt,Rsphere)
! =======================================================

subroutine src2(maxmx,maxmy,num_eqn,num_ghost,mx,my,xlower,ylower, &
dx,dy,q,num_aux,aux,t,dt,Rsphere)

! # Compute source term for Rossby-Haurwitz wave.
! # The source term models the Coriolis force using a 4-stage RK method
! # and the projection of the velocity components to the tangent plane.

implicit none

implicit double precision (a-h,o-z)
dimension q(num_eqn, 1:mx, 1:my)
dimension aux(num_aux, 1:mx, 1:my)
double precision :: RK(4,3)
real(kind=8) :: q(num_eqn, 1:mx, 1:my)
real(kind=8) :: aux(num_aux, 1:mx, 1:my)
real(kind=8) :: RK(4,3)
real(kind=8) :: a, Omega, df, erx, ery, erz, qn, xc, yc, rad, theta
real(kind=8) :: xp, yp, zp, phi, fcor, hu, hv, hw
integer :: num_eqn, num_ghost, mx, my, num_aux, maxmx, maxmy
integer :: i, j, m
real(kind=8) :: xlower, ylower, dx, dy, t, dt, Rsphere

!f2py integer intent(in) maxmx
!f2py integer intent(in) maxmy
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