Line charge density expressed via Dirac delta function

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SUMMARY

The discussion focuses on deriving the surface charge density σ(x,y) from a finite-length wire with a linear charge density λ = Q/L. The attempt to express σ(x,y) using the Dirac delta function δ(y - f(x)) is identified as flawed because it does not account for the correct integration over the wire's geometry. The correct relationship is established as σ(x,y) = λ * δ(y - f(x)) * √(1 + (dy/dx)²), ensuring that the total charge Q is accurately represented when integrating over the surface.

PREREQUISITES
  • Understanding of linear charge density and surface charge density concepts
  • Familiarity with the Dirac delta function and its properties
  • Knowledge of calculus, particularly integration techniques
  • Basic understanding of differential geometry related to curves
NEXT STEPS
  • Study the properties and applications of the Dirac delta function in physics
  • Learn about charge distributions in electrostatics, focusing on surface charge density
  • Explore integration techniques for functions defined on curves in the x-y plane
  • Investigate the relationship between line charge density and surface charge density in different geometries
USEFUL FOR

This discussion is beneficial for physics students, particularly those studying electromagnetism, as well as educators and researchers interested in charge distributions and mathematical modeling of physical systems.

Heirot
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Homework Statement



Let's say we have a wire of finite length L with total charge Q evenly spread along the wire so that lambda=Q/L, linear charge density, is constant. The wire is shaped in x-y plane in some well behaved curve y = f(x). Find the surface charge density sigma(x,y).

Homework Equations



Q = Int(lambda dl) = Int ( Sqrt(1+(dy/dx)^2) dx) for line charge density
Q = Int(sigma(x,y) dx dy) for surface charge density

The Attempt at a Solution



The most logic thing to do would be to write sigma(x,y) = lambda * delta(y-f(x)), where delta(x) is Dirac's delta function. Unfortunately, this doesn't give the right Q, because integration of the delta function over y only give 1 and not the required Sqrt(1+(dy/dx)^2).

Where's the error in reasoning?
 
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But

<br /> \begin{equation*}<br /> \begin{split}<br /> Q &amp;= \lambda L \\<br /> &amp;= \lambda \int \sqrt{1 + \left( \frac{dy}{dx}\right)^2} dx.<br /> \end{split}<br /> \end{equation*}<br />

Heuristically, the amount of charge on the wire between x and x + dx is

dQ = \lambda dL = \lambda \sqrt{1 + \left( \frac{dy}{dx}\right)^2} dx.
 
Last edited:
I agree. So, dQ = sigma(x,y) dx dy. What's sigma(x,y)?
 

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