From charlesreid1

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(Fix math notation error: changed \partial v to \partial n in general boundary condition (v was used for both Sherwood number and normal coordinate). Also fixed Python import (matplotlib.pyplot, not matplotlib.pylab) and explicit iv import. (via update-page on MediaWiki MCP Server))
 
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<math>
<math>
v (1-u_s) = \dfrac{\partial u}{\partial v}
v (1-u_s) = \dfrac{\partial u}{\partial n}
</math>
</math>


Line 51: Line 51:


<source lang="python">
<source lang="python">
import matplotlib.pylab as plt
import matplotlib.pyplot as plt
from scipy.special import *
from scipy.special import iv


# Radial dimension
# Radial dimension
Line 62: Line 62:
# Sherwood number (rate of transfer of material across boundary)
# Sherwood number (rate of transfer of material across boundary)
v = 100.0
v = 100.0
# Create solution vector
y1 = [iv(0,phi*rho) / ( iv(0,phi) + (phi/v)*iv(1,phi) ) for rho in r]
plot(r,y1)


# Create parametric solution vector
# Create parametric solution vector
Line 71: Line 67:
     y = [iv(0,phi*rho) / ( iv(0,phi) + (phi/v)*iv(1,phi) ) for rho in r]
     y = [iv(0,phi*rho) / ( iv(0,phi) + (phi/v)*iv(1,phi) ) for rho in r]
     plt.plot(r,y)
     plt.plot(r,y)
     plt.set_xlabel('r')
     plt.xlabel('r')
     plt.set_ylabel('u')
     plt.ylabel('u')
     plt.hold(True)
     plt.hold(True)
</source>
</source>


which results in a plot of solutions for various Thiele modulii, for a given Sherwood number, shown below:
which results in a plot of solutions for various Thiele modulii, for a given Sherwood number, shown below:
[[Image:BesselFunctionSolutions.png]]




=Flags=


[[Category:Mathematics]]
{{PythonFlag}}
[[Category:Python]]

Latest revision as of 22:59, 14 June 2026

The Problem Setup

I had to deal with some Bessel Functions in dealing with an analytical solution of steady state reaction-diffusion partial differential equation. The diffusion-reaction equation is a simplified, non-dimensionalized equation for a single species and single reaction, and is given by:

$ \nabla^2 u = \phi^2 u $

with the following boundary condition on the boundary of the domain:

$ v (1-u_s) = \dfrac{\partial u}{\partial n} $

For an infinite cylinder (analytical solutions on cylinders typically end up using Bessel Functions), the solution can be written in terms of the non-dimensionalized radial dimension $ \rho $:

$ \dfrac{1}{\rho} \dfrac{d}{d \rho} \left( \rho \dfrac{du}{d \rho} \right) = \phi^2 u $

over the region $ 0 \leq \rho \leq 1 $, and the boundary conditions:

$ \dfrac{du}{d \rho} = 0 $

at $ \rho=0 $, and also

$ v(1-u) = \dfrac{\partial u}{\partial \rho} $

at $ \rho=1 $.

The Solution

The solution to the above equations is given on an infinite cylinder by the equation:

$ u(\rho) = \dfrac{ I_0 (\phi \rho) }{ I_0(\phi) + \frac{\phi}{v} I_1(\phi) } $

where $ I_0 $ and $ I_1 $ are modified Bessel functions of the first kind.

Bessel Functions with Scipy

The Scipy documentation shows you how to call the $ I_v $ modified Bessel functions:

Implementing the solution given above in Python is dead simple:

import matplotlib.pyplot as plt
from scipy.special import iv

# Radial dimension
r = linspace(0,1,100)

# Thiele modulus (ratio of reaction versus diffusion driving forces)
phi = 0.1

# Sherwood number (rate of transfer of material across boundary)
v = 100.0

# Create parametric solution vector
for phi in range(10):
    y = [iv(0,phi*rho) / ( iv(0,phi) + (phi/v)*iv(1,phi) ) for rho in r]
    plt.plot(r,y)
    plt.xlabel('r')
    plt.ylabel('u')
    plt.hold(True)

which results in a plot of solutions for various Thiele modulii, for a given Sherwood number, shown below:

BesselFunctionSolutions.png


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