Integration and Laplacian in polar coordinates

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SUMMARY

The discussion focuses on solving the Laplacian in polar coordinates for an axisymmetric function y(r), specifically addressing the equation ∇²y(r) = Z. The participant correctly applies the Laplacian operator in polar coordinates, simplifying it to ∇² = (1/r)(∂/∂r)(r*(∂/∂r)) due to the absence of θ dependence. The solution involves integrating to find y = (1/4)Z*r² + C ln(r) + K, confirming the procedure is valid by substituting back into the original equation.

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chilge
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Homework Statement


I have a function y that is axisymmetric, so that y=y(r).

I want to solve for r such that ∇2y(r) = Z.

Can anyone tell me if I'm following the right procedure? I'm not sure since there are two "∂/∂r"s present...


Homework Equations


2 = (1/r)(∂/∂r)(r*(∂/∂r)) + (1/r2)*(∂2/∂θ2)
--> The terms involving theta become zero since y is a function of r only


The Attempt at a Solution


2y = (1/r)(∂/∂r)(r*(∂y/∂r)) = Z
(∂/∂r)(r*(∂y/∂r)) = Zr
integrate with respect to r: r(∂y/∂r) = (1/2)Z*r2 + C
(∂y/∂r) = (1/2)Zr + C/r
integrate with respect to r again: y = (1/4)Z*r2 + Cln(r) + K
 
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chilge said:

Homework Statement


I have a function y that is axisymmetric, so that y=y(r).

I want to solve for r such that ∇2y(r) = Z.

Can anyone tell me if I'm following the right procedure? I'm not sure since there are two "∂/∂r"s present...

Homework Equations


2 = (1/r)(∂/∂r)(r*(∂/∂r)) + (1/r2)*(∂2/∂θ2)
--> The terms involving theta become zero since y is a function of r only

The Attempt at a Solution


2y = (1/r)(∂/∂r)(r*(∂y/∂r)) = Z
(∂/∂r)(r*(∂y/∂r)) = Zr
integrate with respect to r: r(∂y/∂r) = (1/2)Z*r2 + C
(∂y/∂r) = (1/2)Zr + C/r
integrate with respect to r again: y = (1/4)Z*r2 + Cln(r) + K

Looks fine to me. If you substitute that back into the original equation you do get Z, right? That's a good way to check.
 
Last edited:

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