Jackson 2.17 on the Laplace equation

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SUMMARY

The discussion focuses on solving the Laplace equation using Jackson 2.17, specifically addressing the equation involving the Green function, \( g_m(\rho, \rho') \). The key difference between the two equations presented lies in the presence of the constant \( \rho' \), which is essential for the Green function. Additionally, the solution varies based on the relationship between \( \rho \) and \( \rho' \), necessitating a method to combine solutions for different regions to account for the delta source term on the right-hand side.

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Homework Statement


I have problems solving the related Laplace equations in the problem


Homework Equations


\frac{1}{\rho}\frac{\partial}{\partial\rho}\rho\frac{\partial g_m(\rho,\rho^')}{\partial\rho}-m^2g_m(\rho,\rho^')}=-4\pi\frac{\delta(\rho-\rho^')}{\rho}


The Attempt at a Solution


My questions are as follows:
1. What's the difference between this equation and \frac{1}{\rho}\frac{\partial}{\partial\rho}\rho\frac{\partial g_m(\rho)}{\partial\rho}-m^2g_m(\rho)=-4\pi\frac{\delta(\rho)}{\rho}?
2. The solution I found on internet suggests that the solution is different when \rho > \rho^' and \rho < \rho^'. Why?
Thanks a lot for your time.
 
Physics news on Phys.org
1. \rho' is just a constant, for the purposes of this equation. You want it in there, because it's needed in the Green function.

2. To find a solution to the equation with the delta source on the rhs, first find the solution with zero on the rhs. You will have some arbitrary constants in the solution. Then, the idea is to take two different solutions and stitch them together such that they produce the delta source term.
 

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