Analytical Solutions for 1D Transient Heat Conduction in Cylindrical Coordinates

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Discussion Overview

The discussion revolves around finding analytical solutions for the 1D transient heat conduction equation in cylindrical coordinates, specifically for a hollow cylinder in an infinite boundary context. Participants are exploring boundary conditions and comparing numerical solutions with analytical approaches.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant has developed a numerical code for the 1D heat equation in cylindrical coordinates and seeks a simple analytical solution for verification.
  • Another participant questions the initial setup, suggesting that for a hollow cylinder, the radius should be treated as a fixed quantity rather than a variable in the temperature equation.
  • A later reply clarifies that the temperature changes are considered only in the radial direction, maintaining the 1D governing equation while noting that boundary conditions differ.
  • One participant mentions finding a solution in the reference book by Carslaw and Jaegar but expresses uncertainty about its correctness.
  • Another participant suggests that the general solutions involve a linear combination of modified Bessel functions and Neumann modified functions, cautioning that Neumann's functions may not be applicable due to divergence at the origin.
  • One participant provides a link to a book solution for 1-D transient heat conduction and mentions working on a separate 2-D problem.

Areas of Agreement / Disagreement

Participants express differing views on the treatment of the hollow cylinder and the applicability of certain mathematical functions. The discussion remains unresolved regarding the correct analytical solution and the appropriate boundary conditions.

Contextual Notes

Participants highlight potential confusion regarding the definitions of the cylinder's geometry and the implications for the governing equations. There are also references to specific mathematical functions that may or may not apply under certain conditions.

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Hi, I have written a numerical code to solve the 1D heat equation in cyclindrical coordinates:

\frac{\partial T}{\partial t}=\kappa\left(\frac{\partial^{2}T}{\partial r^{2}}+\frac{1}{r}\frac{\partial T}{\partial r}\right)

The problem I'm considering is a hollow cylinder in an infinite boundary, i.e. an underground tunnel surrounded by earth. All I want to do is verify that my code is working correctly so to do this I want to find the simplest analytical solution for 1D transient heat conduction using the simplest boundary condition, i.e. constant values. Now if this was in cartesian coordinates I would simply compare it with the solution for a semi infinite approximation. Unfortunately from my research I haven't found an equivalent for cyclindrical coordinates.

I may be missing some here so does anybody have ideas for a simple analytical solution? Thanks.
 
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Hi, I have written a numerical code to solve the 1D heat equation in cyclindrical coordinates:

\frac{\partial T}{\partial t}=\kappa\left(\frac{\partial^{2}T}{\partial r^{2}}+\frac{1}{r}\frac{\partial T}{\partial r}\right)

The problem I'm considering is a hollow cylinder in an infinite boundary, i.e. an underground tunnel surrounded by earth. All I want to do is verify that my code is working correctly so to do this I want to find the simplest analytical solution for 1D transient heat conduction using the simplest boundary condition, i.e. constant values. Now if this was in cartesian coordinates I would simply compare it with the solution for a semi infinite approximation. Unfortunately from my research I haven't found an equivalent for cyclindrical coordinates.

I may be missing some here so does anybody have ideas for a simple analytical solution? Thanks.

I'm not sure you got the equation right: if you are considering hollow cylinder, than r isn't variable of temperature, but a fixed quantity (radius of your pipe) . In an angle-independent case, you should have equation for T (z, t) rather than T (r, t) . Setting situation like that, hollow cylinder shouldn't be unlike standard, exactly solvable 1D case.
 
Sorry, maybe my description isn't quite clear enough. Essentially I'm considering an infinitely long cyclinder, such that I'm only considering temperature changes in the radial direction which is assumed independent of \theta and z. Therefore the 1D governing equation still holds, but the boundary conditions change. It's this bit that I am having trouble with.

In the end I have found a solution in Carslaw and Jaegar but I'm not sure whether it is correct.
 
ads. said:
Sorry, maybe my description isn't quite clear enough. Essentially I'm considering an infinitely long cyclinder, such that I'm only considering temperature changes in the radial direction which is assumed independent of \theta and z. Therefore the 1D governing equation still holds, but the boundary conditions change. It's this bit that I am having trouble with.

In the end I have found a solution in Carslaw and Jaegar but I'm not sure whether it is correct.

Ok than, you confused me mentioning hollow cylinder in opening post - obviously cylinder needs to be solid to consider radial heat conduction. You did get your equation right and general solutions would be linear combination of modified Bessel function of 0th order (because it is angle independent) and Neumann modified functions, it seems. Considering your boundary conditions, where temperature at r = 0 being finite, Neumann's function need not to be considered (they diverge at r = 0) , so all you need is to scale Bessel's functions. But take this cum grano salis, I'm not sure my memory is good on that one :) Good luck!
 

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