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June 7, 2012 02:08
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Fipy: Beer-Lambert law with multiple reflections
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# http://matforge.org/wd15/blog | |
from __future__ import division | |
from fipy import * | |
# Grid things | |
N = 1000 | |
D = 1 | |
dx = D / N | |
m = Grid1D(nx=N, dx=dx) | |
I_right = CellVariable(mesh=m, value=1., name='I_right') # Intensity along the positive direction | |
I_left = CellVariable(mesh=m, value=1., name='I_left') # Intensity along the positive direction | |
# Constants | |
A = 0. | |
B = 1. | |
C = (1 - A) | |
alpha = CellVariable(mesh=m, value=5., name="absorption coefficient") | |
# Constraints --- problem here! | |
I_right.constrain( A * I_left[0] + C, where=m.getFacesLeft()) # x=0 BC | |
I_left.constrain( B * I_right[-1], where=m.getFacesRight()) # x=D BC | |
# Equations to solve | |
eq1 = ExponentialConvectionTerm(var=I_right) + ImplicitSourceTerm(alpha, var=I_right) == 0 | |
eq2 = -ExponentialConvectionTerm(var=I_left) + ImplicitSourceTerm(alpha, var=I_left) == 0 | |
# Beer-lambert (holds when A and B are small) | |
beer_lambert = CellVariable(mesh=m, name='beer_lambert', value=numerix.exp(-alpha * m.x)) | |
# Analytical expression for the differential equation above | |
analytical = CellVariable(mesh=m, name='analytical', value=-( B * numerix.exp( 2 * alpha * m.x ) + numerix.exp( 2 * alpha * D ) ) * C * numerix.exp( -alpha * m.x ) / ( A * B - numerix.exp( 2 * alpha * D ) )) | |
eq = eq1 & eq2 | |
step = 0 | |
while step < 10: | |
print step | |
res= eq.sweep() | |
step += 1 | |
vi = Viewer(vars=(beer_lambert, analytical, I_left + I_right)) | |
#vi = Viewer(vars=(I_left + I_right)) | |
vi.plot(filename='light_A=0,B=1.png') | |
raw_input() |
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There is an issue with setting boundary conditions correctly in this example -- don't use!