Solution of diffusion equation with three independent variable (r,z,t)

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The discussion focuses on solving a diffusion equation with three independent variables: r, z, and t, specifically for a concentration C in an axisymmetric tube. The equation is expressed in cylindrical coordinates, simplifying the Laplacian operator due to the assumption of axial symmetry. A recommended approach is to seek separable solutions of the form C(r,z,t) = R(r)Z(z)T(t), which allows the equation to be divided into ordinary differential equations for each variable. The solution can then be constructed as a sum of these separated solutions, tailored to the given initial and boundary conditions. This method provides a structured way to tackle the diffusion problem in the specified geometry.
nazmulislam
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Hi,

I want to solve the following diffusion equation:

(d/dt) C(r,z,t)=D*∇^2 C(r,z,t)

where C is the concentartion and D is the coefficient of diffusivity (constant)

with initial condition C(r,z,0)=C0 (constant)
and boundary condition dc/dr=0 at r=0; (dc/dz) at z=-L equal to (dc/dz) at z=L

where I have considered axisymmetric tube of length L.

Can anybody help to solve the above mentioned problem for the concentration C?
 
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Since you are using "symmetric tube" you will probably want to use "cylindrical coordinates", suppressing the \theta dependence. In cylindrical coordinates the Laplacian is
\nabla^2 f= \frac{\partial^2 f}{\partial r^2}+ \frac{1}{r}\frac{\partial f}{\partial r}+ \frac{\partial^2 f}{\partial \theta^2}+ \frac{\partial^2 f}{\partial z^2}

Assuming "axially symmetric" so f does not depend on \theta, that is
\nabla^2 f= \frac{\partial^2 f}{\partial r^2}+ \frac{1}{r}\frac{\partial f}{\partial r}+ \frac{\partial^2 f}{\partial z^2}

So your equation says
\frac{\partial C}{\partial t}= D\left(\frac{\partial^2 C}{\partial r^2}+ \frac{1}{r}\frac{\partial C}{\partial r}+ \frac{\partial^2 C}{\partial z^2}\right)

A standard method of solving that is to look for "separable solutions". That is, look for solutions of the from C(r,z,t)= R(r)Z(z)T(t). That will separate the equation into ordinary differential equations for R, Z, and T separately. Depending on the boundary and initial conditions, the solution can be written as a sum of such "separated" solutions.
 
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Thanks Hallsoflvy for your nice explanation.
 

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