Laplace equation, cylindrical 2D

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Homework Help Overview

The discussion revolves around the Laplace equation in cylindrical coordinates, specifically focusing on the assumed solution form u(rho, Phi) = rho^n * Phi(phi). Participants are exploring the implications of this assumption and the steps involved in deriving the general solution.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss the validity of the assumed solution and question the differentiation process with respect to rho. There is an exploration of the substitution of u(rho, Phi) into Laplace's equation and the resulting expressions. Some participants express confusion regarding the correctness of their manipulations and the conditions under which the solution holds.

Discussion Status

The discussion is active, with participants providing feedback on each other's attempts and clarifying points of confusion. There is acknowledgment of errors in expressions and a collaborative effort to correct them. Some participants indicate that they have reached a better understanding of the problem through this dialogue.

Contextual Notes

Participants note a transition from cylindrical to plane polar coordinates, which introduces additional considerations in their calculations. There is an emphasis on ensuring the correct application of the Laplace equation in the context of these coordinate systems.

Niles
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[SOLVED] Laplace equation, cylindrical 2D

Homework Statement


I am given the Laplace eq. in cylindrical coord. (2D), and I am told that we can assume the solution u(rho, Phi) = rho^n * Phi(phi).

Find the general solution.

The Attempt at a Solution


My teacher says that the general solution is u(rh,Phi) = SUM [A*cos(...) + B*sin(...)]*rho^n.

It is tis version of the Laplace equation on the first equation on page 12 in here:

http://people.ifm.liu.se/boser/elma/Lect4.pdf

Why do we not differentiate rho?
 
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Niles said:

Homework Statement


I am given the Laplace eq. in cylindrical coord. (2D), and I am told that we can assume the solution u(rho, Phi) = rho^n * Phi(phi).

Find the general solution.

The Attempt at a Solution


My teacher says that the general solution is u(rh,Phi) = SUM [A*cos(...) + B*sin(...)]*rho^n.

It is tis version of the Laplace equation on the first equation on page 12 in here:

http://people.ifm.liu.se/boser/elma/Lect4.pdf

Why do we not differentiate rho?

You do differentiate with respect to rho! Just plug in the general solution and you will see that it works, at the condition of choosing the constant inside the trig function correctly . You cannot put any old constant multiplying phi inside the trig function.
write the argument of the trig function as c \phi and plug the general solution in Laplace's equation and you will see that it does work at the condition of choosing "c" to be some particular value (in terms of "n").
 
Ok, now I have substituted u(rho,Phi) in Laplaces equation, divided through by rho^n*Phi and multiplied by rho^2:<br /> \frac{\rho }{{\rho ^n }}\frac{\partial }{{\partial \rho }}\left( {\rho \frac{{\partial \rho ^n }}{{\partial \rho }}} \right) + \frac{1}{\Phi }\frac{{\partial ^2 \Phi }}{{\partial \phi ^2 }} = 0<br />

The rho-part does not equal rho^n. Or am I wrong here?
 
Niles said:
Ok, now I have substituted u(rho,Phi) in Laplaces equation, divided through by rho^n*Phi and multiplied by rho^2:


<br /> \frac{\rho }{{\rho ^n }}\frac{\partial }{{\partial \rho }}\left( {\rho \frac{{\partial \rho ^n }}{{\partial \rho }}} \right) + \frac{1}{\Phi }\frac{{\partial ^2 \Phi }}{{\partial \phi ^2 }} = 0<br />

The rho-part does not equal rho^n. Or am I wrong here?

Look again at the laplacian in cylindrical coordinates. There are two mistakes in the expression you wrote above!
 
Duh, I meant plane polar, not cylindrical - sorry!

So the above is written in plane polar, but it still doesn't work.

EDIT: The only thing that changes when going to plane polars from cylindrical is that the z-part is missing. So that counts for one of the errors. So one error is remaining, but there is none?
 
Last edited:
This is what you want.
<br /> <br /> \rho \frac{\partial }{{\partial \rho }}\left( {\rho \frac{{\partial \Phi }}{{\partial \rho }}} \right) + \frac{{\partial ^2 \Phi }}{{\partial \phi ^2 }} = 0<br /> <br />

Just take the cylindrical form, drop z and multiply by rho^2. It does work.
 
By doing that, I get {\frac{\rho}{\rho ^n} \frac{\partial }{{\partial \rho }}\left( {\rho \frac{{\partial \rho ^n}}{{\partial \rho }}} \right) + \frac{1}{\Phi}\frac{{\partial ^2 \Phi }}{{\partial \phi ^2 }} = 0.<br /> <br /> <br />

What I did was to insert u(rho, Phi) = rho^n*Phi in the expression Dick wrote to the right of the partial d's, right? Then I divide by rho^n and Phi, and the above expression is what I end up with.

EDIT: Yeah, it really does work. Thanks to both of you!
 
Last edited:

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