Converting volume elements to area elements

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SUMMARY

The discussion focuses on evaluating the integral of the form h(𝑥) = ∫ d³𝑥' (δ(r' - R) / |𝑥 - 𝑥'|), where r' = |𝑥'|. The integral represents the electrostatic potential of a charged spherical shell, with the delta function δ(r' - R) acting as a charge density restricted to the shell's surface. The user seeks a rigorous method to convert the volume integral with the delta function into a surface integral without relying on physical intuition. The divergence theorem is mentioned as a potential tool for this conversion, although the user expresses uncertainty about its application in this context.

PREREQUISITES
  • Understanding of delta functions in integrals
  • Familiarity with electrostatic potential and charge distributions
  • Knowledge of spherical coordinates in calculus
  • Comprehension of the divergence theorem in vector calculus
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  • Study the application of the divergence theorem in converting volume integrals to surface integrals
  • Explore Griffiths' "Introduction to Electrodynamics" for examples on electrostatic potential calculations
  • Learn about the properties and applications of delta functions in physics
  • Investigate techniques for evaluating integrals involving singularities and distributions
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Students of physics, particularly those studying electromagnetism, mathematicians dealing with integrals involving delta functions, and anyone interested in the rigorous treatment of charge distributions in electrostatics.

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Homework Statement



I need to evaluate an integral of the form:

h(\vec{x}) = \int d^3\vec{x}' \frac{\delta(r' - R)}{|\vec{x}-\vec{x}'|}

where r' = |\vec{x}'| = \sqrt{x'^2 + y'^2 + z'^2}.

Homework Equations



The above, and maybe the fact that \delta(g(x)) = \sum_i \frac{\delta(x - x_i)}{|g'(x_i)|} where x_i are the roots of g.

The Attempt at a Solution



I can solve the problem with some physical motivation as follows:

The given integral is the same as what you would do if you wanted to calculate the electrostatic potential of a charged spherical shell: V(\vec{x}) = \frac{1}{4\pi\epsilon_0}\int d\tau' \frac{\rho(\vec{x}')}{|\vec{x}-\vec{x}'|} where d\tau is the volume element and \rho(\vec{x}') = \delta(r' - R). In this case, the delta function restricts the "charge density" rho to the surface of the shell. The same physical problem can be treated with the formula for the electrostatic potential of a surface charge distribution: V(\vec{x}) = \frac{1}{4\pi\epsilon_0}\int da' \frac{\sigma(\vec{x}')}{|\vec{x}-\vec{x}'|} where da is the area element and, in this case, we can take \sigma = 1. This integral can now be computed straightforwardly in spherical coordinates, e.g. Griffiths "Introduction to Electrodynamics" example 2.7, yielding h(\vec{x}) = 4\pi R^2 / |\vec{x}|.

However, I would like to be able to do this calculation without having to use physical intuition to interpret a volume integral with a delta function as being equivalent to a surface integral without the delta function; that is, I just want to explicitly integrate out one of x,y, or z with the delta function and then go from there. How do I do this? I've tried using the equation I gave in (2), but it just produces a giant mess from which I don't know how to proceed.

I guess an equivalent question would be: given the expression above for the electrostatic potential of a volume distribution (which is really a surface dist.) of charge with \rho(\vec{x}) = \sigma \cdot \delta(f(\vec{x})), how do you rigorously derive the expression for a surface distribution?
 
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It sounds like you need the "divergence theorem":
\int\int_V\int \nabla\cdot \vec{f} dV= \int_S\int \vec{f}\cdot d\vec{S}
where S is the surface bounding volume V.
 
Can you expand on that? I know what the divergence theorem is, but there are no divergences in this problem. My question isn't: "given an integral over a region, how do you convert it to an integral on the boundary"? It's: "given an integral over all space but over a delta function, how do you convert it to an integral without the delta function over the surface that the delta function restricts to?"
 

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