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135 changes: 135 additions & 0 deletions pyro/multigrid/axisymmetric_MG.py
Original file line number Diff line number Diff line change
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r"""
A multigrid solver for axisymmetric coordinates (r-z) to solve
an elliptic equation of the form:

L \phi = f

where L is the Laplacian operator in cylindrical coords.
"""

import matplotlib.pyplot as plt
import numpy as np
import pyro.mesh.array_indexer as ai
from pyro.multigrid import MG

np.set_printoptions(precision=3, linewidth=128)


class AxisymmetricMG2d(MG.CellCenterMG2d):

def __init__(self, nx, ny, xmin=0.0, xmax=1.0, ymin=0.0, ymax=1.0,
xl_BC_type="reflect", xr_BC_type="dirichlet",
yl_BC_type="dirichlet", yr_BC_type="dirichlet",
xl_BC=None, xr_BC=None,
yl_BC=None, yr_BC=None,
nsmooth=10, nsmooth_bottom=50,
verbose=0,
true_function=None, vis=0, vis_title=""):

# initialize the MG object with the auxillary "coeffs" field
MG.CellCenterMG2d.__init__(self, nx, ny, ng=1,
xmin=xmin, xmax=xmax, ymin=ymin, ymax=ymax,
xl_BC_type=xl_BC_type, xr_BC_type=xr_BC_type,
yl_BC_type=yl_BC_type, yr_BC_type=yr_BC_type,
xl_BC=xl_BC, xr_BC=xr_BC,
yl_BC=yl_BC, yr_BC=yr_BC,
nsmooth=nsmooth, nsmooth_bottom=nsmooth_bottom,
verbose=verbose,
true_function=true_function, vis=vis,
vis_title=vis_title)

def smooth(self, level, nsmooth):
"""
Use red-black Gauss-Seidel iterations
"""

v = self.grids[level].get_var("v")
f = self.grids[level].get_var("f")

self.grids[level].fill_BC("v")

myg = self.grids[level].grid

dr = myg.dx
dz = myg.dy

rc = ai.ArrayIndexer(myg.x2d, grid=myg)
rl = rc - 0.5 * dr
rr = rc + 0.5 * dr

denom = 2 * (1.0 / dr**2 + 1.0 / dz**2)

# do red-black G-S
for _ in range(nsmooth):

# do the red black updating in four decoupled groups
#
#
# | | |
# --+-------+-------+--
# | | |
# | 4 | 3 |
# | | |
# --+-------+-------+--
# | | |
# jlo | 1 | 2 |
# | | |
# --+-------+-------+--
# | ilo | |
#
# groups 1 and 3 are done together, then we need to
# fill ghost cells, and then groups 2 and 4

for n, (ix, iy) in enumerate([(0, 0), (1, 1), (1, 0), (0, 1)]):

v.ip_jp(ix, iy, s=2)[:, :] = (-f.ip_jp(ix, iy, s=2) +
1.0 / (rc.ip(ix, s=2) * dr**2) * (rr.ip(ix, s=2) * v.ip_jp(1+ix, iy, s=2) +
rl.ip(ix, s=2) * v.ip_jp(-1+ix, iy, s=2)) +
1.0 / dz**2 * (v.ip_jp(ix, 1+iy, s=2) + v.ip_jp(ix, -1+iy, s=2))) / denom

if n in (1, 3):
self.grids[level].fill_BC("v")

if self.vis == 1:
plt.clf()

plt.subplot(221)
self._draw_solution()

plt.subplot(222)
self._draw_V()

plt.subplot(223)
self._draw_main_solution()

plt.subplot(224)
self._draw_main_error()

plt.suptitle(self.vis_title, fontsize=18)

plt.draw()
plt.savefig("mg_%4.4d.png" % (self.frame))
self.frame += 1

def _compute_residual(self, level):
""" compute the residual and store it in the r variable"""

v = self.grids[level].get_var("v")
f = self.grids[level].get_var("f")
r = self.grids[level].get_var("r")

myg = self.grids[level].grid

dr = myg.dx
dz = myg.dy

rc = ai.ArrayIndexer(myg.x2d, grid=myg)
rl = rc - 0.5 * dr
rr = rc + 0.5 * dr

# compute the residual
# r = f - L_eta phi
L_phi = (1.0 / (rc.v() * dr**2) * (rr.v() * v.ip(1) - 2.0 * rc.v() * v.v() + rl.v() * v.ip(-1)) +
1.0 / (dz**2) * (v.jp(1) - 2.0 * v.v() + v.jp(-1)))

r.v()[:, :] = f.v() - L_phi
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