Conductor that can completely surround another conductor?

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Homework Help Overview

The discussion revolves around demonstrating that the capacitance of any conductor is always smaller than or equal to that of a conductor which can completely surround it. The subject area includes concepts of capacitance and electrostatics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the definition of capacitance in relation to one or two conductors, questioning how to demonstrate the relationship between the capacitance of a conductor and that of a surrounding conductor. They discuss the implications of charge distribution and potential differences.

Discussion Status

Participants are actively engaging with the problem, offering insights and asking clarifying questions. Some guidance has been provided regarding the relationship between potential differences and capacitance, but explicit consensus on a method or solution has not been reached.

Contextual Notes

There are indications of assumptions regarding the definition of capacitance and the configuration of conductors involved. Participants are also considering the implications of conductor size and shape on capacitance.

merrypark3
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Homework Statement


"demonstrate that the capacitance of any conductor is always smaller than or equal to the capacitance of a conductor which can completely surround it"


Homework Equations



Multipole expansion?


The Attempt at a Solution



Tried to compare each terms of pole-moments of the distribution...
 
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Usually, capacitance is defined in terms of two conductors, one with charge +Q and the other with charge -Q. The capacitance then is the ratio Q/ΔV, where ΔV is the potential difference between the two conductors. I assume that by the "capacitance of a conductor" is meant one of the conductors is at infinity. So look at two conductors, one larger than the other, bearing the same charge Q and compare the ratio Q/ΔV, where ΔV is the potential difference between a given conductor and infinity.
 
I think the capacitance in this problem is defined in terms of one conductor.
If a conductor of spherical shell of radius R is charged with Q, then the potential is Q/R so the capacitance is R.
So If we limit the case to a concentric spherical shell, then obviously the small one has small capacitance. But for any shape of conductor? How can I demonstrate? I've tried with mutipole expansion, but ,...
Please help me
 
I will help you, but you have to read and understand what I post. Imagine an irregular conductor, call it A, that has charge Q on it. It is an equipotential, but there is potential difference ΔVA between it and infinity. Its capacitance is CA = Q/ΔVA. Now imagine a second conductor, B, that can completely surround conductor A if called upon to do so. Put the same amount of charge Q on conductor B. It too is an equipotential and its capacitance will be CB = Q/ΔVB. If you can demonstrate that ΔVB is less than ΔVA, then you have answered the question.
 
Yes, that's right. But, How can I demonstrate that ΔVB is less than ΔVA..
 
What happens to the potential on conductor B in the limit that its size becomes infinitely large?
 
zero. I have thought about that. But considering only that case is not enough?
 
No it is not. What will happen if you bring the boundaries of the huge conductor closer in from infinity. Will its potential rise or fall? What if after that you brought the boundaries in even closer?
 
the more closer the potential increases. but that process preserves the shape..
 
  • #10
merrypark3 said:
the more closer the potential increases. but that process preserves the shape..
I don't know what you mean by this or why it is relevant. You have enough information (and help) to answer the question. Just put it together.
 

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