Field inside a cavity inside a conductor

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Homework Help Overview

The discussion revolves around the behavior of electric fields within a cavity inside a conductor, particularly when point charges are introduced into the cavity. The subject area includes electrostatics and the properties of conductors, as well as the implications of the uniqueness theorem and Laplace's equation.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants explore the implications of introducing point charges into a cavity within a conductor and question whether the uniqueness theorem applies in this scenario. There are discussions about the satisfaction of Laplace's equation and the uniqueness of the potential function derived from Poisson's equation.

Discussion Status

Participants are actively engaging with differing viewpoints regarding the application of the uniqueness theorem and the behavior of the electric potential within the conductor. Some guidance has been offered regarding the uniqueness of the potential, but there remains a lack of consensus on the implications of the introduced charges.

Contextual Notes

There are references to Earnshaw's theorem and the stability of the system with point charges, indicating that assumptions about the system's behavior are under scrutiny. The discussion also highlights the importance of boundary conditions and the nature of the electric potential within the conductor.

Kolahal Bhattacharya
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In the context of properties of conductor & 1st Uniqueness theorem, Griffiths proves that field inside a cavity( empty of charge) within a conductor is 0.
Is the result same if we place a +q & a -q (so that Q(enc)=0)
suspended in air inside the cavity?
 
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I would say no, because Laplace's equation won't be satisfied everywhere, because of the point charges. So you can't apply the first uniqueness theorem.
 
I agree with you about the result but cannot be satisfied with your argument.As Poisson's eqn. takes into consideration Rho(r)...& still satisfies Uniqueness theorems. Lastly I think it is solved:we will have a unique V(r) function from which E follows.This V(r) will not satisfy properti--es of Laplace eqn.In boundary, V(r)=V(0),Following properties of a conductor...Otherwise the system I'm talking of will not exist at all.It will collapse immediately after we place them together within the cavity,following Earnshaw's theorem.Any conceptual mistake?Please help!
 
Yeah, you're right, the uniqueness theorem still holds and the potential can be uniquely determined, but it won't be constant inside the conductor.

Also, I don't understand why you say V(R) = V(0)?
 
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