Gauss' Law -- is there a general proof for all geometries?

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SUMMARY

Gauss's Law, represented by the equation Θ=Q/εo, holds true for point charges and spherical surfaces, but the discussion explores the need for a general proof applicable to all charge distributions and geometrical shapes, including cylinders and cubes. The participants emphasize the complexity of deriving Gauss's Law for non-spherical geometries and the necessity of vector calculus and the Dirac delta function for such proofs. A specific reference is made to a lecture that addresses the generalization from spherical surfaces to arbitrary surfaces, highlighting the challenges in calculating electric flux for different shapes.

PREREQUISITES
  • Understanding of Gauss's Law and its application to point charges
  • Familiarity with vector calculus
  • Knowledge of the Dirac delta function
  • Concept of electric flux and its calculation
NEXT STEPS
  • Study the generalization of Gauss's Law for arbitrary surfaces
  • Learn about the application of vector calculus in electromagnetism
  • Research the Dirac delta function and its role in charge distributions
  • Examine electric flux calculations for cylindrical and cubic geometries
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Students of electromagnetism, physicists, and educators seeking to deepen their understanding of Gauss's Law and its applications across various geometries.

davidbenari
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I know how to derive Gauss's law considering only one point charge and a sphere.

I've seen other derivations for other geometrical shapes and I would say this is way too tedious as a method to prove that Gauss's law always holds true.

I was wondering if there is a general proof that says this has to be the case for all charge distributions and all geometrical shapes? Namely,

Θ=Q/εo holds true always.

Also, I'm not looking for proofs that refer to the fact that the "irregular shape is equivalent or reducible to the spherical case". I'm considering cylinders, cubes, and other polygons which as far as I know are not reducible to the spherical case.

Thanks.
 
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If you draw your gaussian surface big enough, not matter what object/shape is inside, it will be comparatively small enough to be assumed a point source.

I don't think there is proof that anything always holds true.
 
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http://farside.ph.utexas.edu/teaching/em/lectures/node30.html

This covers both the generalization from a spherical surface of integration to an arbitrary surface, and from point charges to arbitrary charge distributions. Warning: requires vector calculus, and you'll have to learn about the Dirac delta "function".
 
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Elegysix:

I liked what you said however:

suppose you're calculating flux out of a charged long rod and create a gaussian surface (sphere in this case) so big such that the rod can be consider a point charge. This makes the calculations not simple at all because the electric field is not always parallel to the differential of area on your spherical surface. This is because the electric field on a charged long rod is mostly radial and outwards.

It's important to consider just the sphere in this case because this is would be the basis for a general proof because of its simplicity. So I wouldn't be convinced by "consider a gaussian cylinder then".

Thanks by the way, I didn't think of what you said.
 

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