Electric Field Above a Small Hole in a Charged Spherical Shell?

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SUMMARY

The discussion focuses on calculating the electric field above and below a small hole in a charged spherical shell with radius 'a' and surface charge density 'sigma'. It is established that the electric field below the hole is zero due to Gauss' law, as the charge enclosed remains unchanged. For the electric field above the hole, the approach involves modeling the electric potential, which remains largely unchanged despite the hole, and then using its gradient to derive the electric field. The discussion emphasizes the complexity of integrating over the surface charge when spherical symmetry is disrupted.

PREREQUISITES
  • Understanding of Gauss' law in electrostatics
  • Familiarity with electric potential and its relationship to electric fields
  • Basic calculus for integrating over surface charges
  • Knowledge of spherical symmetry in electric fields
NEXT STEPS
  • Study electric potential and its application in electrostatics
  • Learn advanced integration techniques for surface charge distributions
  • Explore the implications of breaking spherical symmetry in electric field calculations
  • Review examples of electric field calculations involving holes in charged surfaces
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Students of electromagnetism, physicists dealing with electrostatic problems, and educators looking to explain the effects of surface charge modifications on electric fields.

mahorka
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Hey. I am trying to solve the following problem:

Given a spherical shell with radius a and charge density sigma. If a very small patch of this surface were removed, leaving a small hole, what is the electric field just above and just below this hole?

For the electric field below the hole, I think the answer is zero, by gauss' law. Since the charge enclosed would be zero (same as if the hole were not present).

However, I'm not sure how I would go about solving for the electric field above the hole. I initially thought that I could simply calculate what the field would be if the hole was not there, and then take this result and subtract the electric field of a small disk of radius a (that would represent the hole) but I don't seem to get the right answer.

And help would be appreciated! Thanks!
 
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Hello mahorka,

Welcome to Physics Forums!

Have you studied electric potential yet? This problem will be a lot easier if you start by modeling the potential (the potential can be shown to be more or less unchanged whether the small hole is there or not). Then use its gradient to obtain the electric field.

If you don't have the luxury of using potentials, the only way I can think of doing this involves some pretty nasty calculus integrating over the surface charge, treating the surface charges as infinitely small point charges. The thing that makes this tough is you don't get to use the normal equations since spherical symmetry is lost, and the point of interest is not at the origin, but instead somewhere near the surface of the shell. This way of solving the problem is possible, yet brutal.

[Edit]: Btw, I suspect the problem might simply be asking for a verbal explanation rather than an explicit proof. Using the concept of electric potential may allow you to verbally explain what impact the hole would have, if any (without having to show the math). Or you could show the math. But potentials will make it easier either way.
 
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