Electric field of periodic charge density.

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SUMMARY

The discussion focuses on calculating the electrostatic field and potential generated by a two-dimensional charge density described by the function ρ sin(kx) cos(ky) δ(z) at a distance d from the plane z=0. Participants emphasize the necessity of employing Fourier analysis to evaluate the integral required for extending the solution from point charges to two-dimensional charge distributions. The differential form of Gauss's law, ∇·E = ρ/ε₀, serves as a foundational equation in the analysis. The use of Poisson's equation is also highlighted as a critical step in determining the potential through oscillating functions.

PREREQUISITES
  • Understanding of electrostatics and Gauss's law
  • Familiarity with Fourier analysis techniques
  • Knowledge of Poisson's equation in electrostatics
  • Concept of delta functions in charge distributions
NEXT STEPS
  • Study the application of Fourier transforms in electrostatics
  • Learn about solving Poisson's equation for various charge distributions
  • Explore the implications of delta functions in three-dimensional charge density problems
  • Investigate the relationship between charge density and electric field using integral calculus
USEFUL FOR

Students and professionals in physics, particularly those specializing in electromagnetism, as well as researchers working on electrostatic field calculations and Fourier analysis applications.

JoshThompson42
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Homework Statement


Find electrostatic field and potential created by a two-dimensional charge density:
\rho \sin (kx) \cos (ky) \delta (z)
at the distance d from the the plane z=0 where the charge is placed (taking into account that it is embedded in a three dimensional space).
In your calculations you are required to use Fourier analysis.

Homework Equations

The Attempt at a Solution


My initial thought was to use the differential form of Gauss's law:
\nabla \cdot E = \frac{\rho}{\epsilon_0}

However I am unsure of where Fourier analysis comes into play, any pointers as to where to go from here would be great. My instinct tells me that the delta function should be what gets the Fourier treatment, however it isn't periodic.
 
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What is the potential for a point-charge? To extend this to 2-dimensional charge distributions, you'll need an integral. And I guess the evaluation of this integral will need Fourier analysis.
 
mfb said:
What is the potential for a point-charge? To extend this to 2-dimensional charge distributions, you'll need an integral. And I guess the evaluation of this integral will need Fourier analysis.
To make Fourier analysis more obvious, I would start from Poisson's equation for the potential: given the charge distribution, you have to guess oscillating functions for the x and y components which leads to Fourier analysis to determine the coefficients. The z-component is less obvious though, and you'd have to use the ±z symmetry of the problem... Incidentally, the full solution for arbitrary z comes rather easily using Fourier transform.
 

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