How Do You Solve Poisson's Equation Using Fourier Transforms?

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SUMMARY

This discussion focuses on solving Poisson's equation, \(\bigtriangledown^2 \psi(\vec{r}) = \frac{- \rho (\vec{r})}{\epsilon_0}\), using Fourier transforms. The first part involves taking the Fourier transform of both sides, leading to the equation \(-\vec{k}^2 \Psi(\vec{k}) = \frac{-1}{\epsilon_0} P(\vec{k})\). The solution for the Fourier transform of \(\psi(\vec{r})\) is given by \(\Psi (\vec{k}) = \frac{1}{\epsilon_0 \vec{k}^2} P (\vec{k})\). The next step involves applying the inverse transform using the convolution theorem in three dimensions.

PREREQUISITES
  • Understanding of Fourier transforms, specifically in three dimensions.
  • Familiarity with Poisson's equation and its physical significance.
  • Knowledge of the convolution theorem in the context of Fourier analysis.
  • Basic proficiency in vector calculus and differential equations.
NEXT STEPS
  • Study the application of the convolution theorem in three-dimensional Fourier transforms.
  • Learn about the physical interpretations of solutions to Poisson's equation.
  • Explore advanced techniques in Fourier analysis, including properties of Fourier transforms.
  • Investigate numerical methods for solving partial differential equations like Poisson's equation.
USEFUL FOR

Students and professionals in physics, applied mathematics, and engineering who are working on problems involving partial differential equations and Fourier analysis.

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Homework Statement


Solve Poisson's equation, [tex]\bigtriangledown^2 \psi(\vec{r}) = \frac{- \rho (\vec{r})}{\epsilon_0}[/tex], by the following sequence of operations:

a) Take the Fourier transform of both sides of this equation. Solve for the Fourier transform of [tex]\psi(\vec{r})[/tex].
b) Carry out the inverse transform by using a three-dimensional analog of the convolution theorem.

Homework Equations


Fourier transformation

The Attempt at a Solution



I'm working on part a. I understand how to do a Fourier transform, but not so much in 3D. This is my work, I just want to make sure that I've done part a correctly so that I can move on to part b.

[tex]\bigtriangledown^2 \psi(\vec{r}) = \frac{- \rho (\vec{r})}{\epsilon_0}[/tex]
[tex]\frac{-\vec{k}^2}{\sqrt{2\pi}} \int^\infty_{-\infty} \psi(\vec{r}) e^{i \vec{k} \cdot \vec{r}} d\vec{r} = \frac{-1}{\epsilon_0 \sqrt{2\pi}} \int^\infty_{-\infty} \rho (\vec{r}) e^{i \vec{k} \cdot \vec{r}} d\vec{r}[/tex]
[tex]-\vec{k}^2 \Psi(\vec{k}) = \frac{-1}{\epsilon_0} P(\vec{k})[/tex]
[tex]\Psi (\vec{k}) = \frac{1}{\epsilon_0 \vec{k}^2} P (\vec{k})[/tex]
 
Last edited:
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seems ok...
 

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