Does Coulomb's Law apply to more than point charges?

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Discussion Overview

The discussion revolves around the applicability of Coulomb's Law beyond point charges, exploring its relevance to larger charge distributions, such as uniformly charged spheres and other geometries. Participants also touch on related concepts like Gauss's Law and Newton's shell theorem, as well as the implications for experimental setups involving charged objects.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants assert that Coulomb's Law is fundamentally defined for point charges, while others suggest it can apply to spherically symmetric charge distributions under certain conditions.
  • There is a proposal that for large bodies, one must integrate the forces exerted on differential volumes, implying a more complex application of Coulomb's Law.
  • Some participants mention that Newton's shell theorem can be used in conjunction with Coulomb's Law for spherically symmetric charges.
  • Others argue that Gauss's Law is necessary for more general charge distributions, emphasizing that Coulomb's Law is essentially a specific case of Gauss's Law.
  • Concerns are raised about the uniformity of charge distribution on conductive versus dielectric spheres, with some participants questioning the ease of achieving uniform charge on dielectric materials.
  • A hypothetical scenario is posed regarding the implications of Coulomb's Law if two point charges were at zero distance apart, leading to discussions about infinite forces.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of Coulomb's Law to non-point charges, with some asserting it only applies to point charges and others suggesting it can be extended to certain symmetrical configurations. The discussion remains unresolved regarding the broader applicability of Coulomb's Law.

Contextual Notes

Participants mention limitations in applying Coulomb's Law to non-point charges, including the need for integration in complex geometries and the dependence on charge distribution uniformity. There are also unresolved questions about the historical context of Coulomb's experiments and the assumptions made in applying these laws.

Ralphonsicus
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I read an article on Coulomb's law which read, ''Coulomb's law only applies to point charges'' (or something along those lines). Am I wrong, or is there an equivalent that can work for magnets/big electric charges?
 
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IMO, which doesn't actually counts, I think coulomb's law in applicable only to charges which are smaller than the distance between them.
And Coulomb's law is there in electrostatics. You might read more about magnetic field and forcehttp://electron9.phys.utk.edu/phys136d/modules/m7/magnetic.htm.
 
Yes, Coulomb's law is basically defined for point charges. For large bodies, one needs to integrate the partial forces exerted on differential volumes of the bodies.

However,for uniformly charged spheres or spherical shells ( due to symmetry ) , Coulomb's law can be readily used by inserting the distance between the centers of the sphere in the formula. This may be proved by integration but it seems difficult to me. I have a simple and interesting proof for it based on Newton's third law though.
 
Last edited:
Ralphonsicus said:
Am I wrong, or is there an equivalent that can work for magnets/big electric charges?
You are correct, Coulomb's law only works for point charges. If you have a spherically symmetric charge then you can use Newton's shell theorem in conjunction with Coulomb's law to get the force. For more general distributions of charge you need to use Gauss' law. Coulomb's law is essentially Gauss' law evaluated for a point charge.
 
And of course Gauss's Law, while always true, is usable in practice only for certain very symmetrical shapes of charge configurations. For other shapes (e.g. a cylindrical rod of finlte length) you have to integrate Coulomb's Law after dividing up the shape into a lot of infinitesimally small sections which each act like a point charge, at different distances from the point at which you want the field.

A few days ago I had to work out the electric field at a distance z above the center of a thin square sheet of side a, with uniform charge density. I ended up with about three pages of math, setting up and solving a double integral.
 
DaleSpam said:
You are correct, Coulomb's law only works for point charges. If you have a spherically symmetric charge then you can use Newton's shell theorem in conjunction with Coulomb's law to get the force. For more general distributions of charge you need to use Gauss' law. Coulomb's law is essentially Gauss' law evaluated for a point charge.

I wonder if Coulomb made his experiment with uniformly charged spheres. And also if he knew about the Newton's shell theorem. Otherwise he couldn't postulate the law precisely.
 
Hassan2 said:
I wonder if Coulomb made his experiment with uniformly charged spheres. And also if he knew about the Newton's shell theorem. Otherwise he couldn't postulate the law precisely.
Yes, he made his experiment with charged spheres. I am pretty sure that he knew about Newton's shell theorem since it had been in existence for quite some time by then.
 
DaleSpam said:
Yes, he made his experiment with charged spheres. e time by then.

Thanks for the reply.

To my knowledge,Van de graff generators charge conducting spheres rather than dielectric ones. When two conductive spheres are placed near together, the surface charge distribution is not uniform anymore. Am I wrong?

It's not that easy to charge dielectric spheres uniformly or perhaps there are effective ways to do this which I'm not aware of.

Thanks again.
 
I am not aware of the details of the charged spheres. I am sure if you looked you could find Coulomb's description of the experiment. Given the accuracy of measuring forces I doubt that the details of the charge distribution were the dominant source of error in his experiment.
 
  • #10
Hypothetical question:

If two oppositely charged point charges have a distance between them of 0 m, how could they be separated; Coulomb's Law would indicate that the electric force between the charges would be an infinite amount of Newtons?
 

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