Potential of a conducting sphere with charge inside

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SUMMARY

The electric potential of a hollow neutral conducting sphere with radius R, containing a charge q inside, is consistently q/R regardless of the charge's position within the sphere. This constancy arises from the uniform charge distribution on the sphere's surface, which remains unchanged by the internal charge's location. The potential outside the sphere is determined by the total charge enclosed, leading to the conclusion that the potential at any point outside the sphere is equivalent to that of a point charge located at the center.

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  • Understanding of electrostatics principles
  • Familiarity with electric potential and charge distribution
  • Knowledge of Gaussian surfaces in electrostatics
  • Basic concepts from Griffiths' "Introduction to Electrodynamics"
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  • Explore the implications of charge distribution on conducting surfaces
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Students of physics, particularly those studying electrostatics, educators teaching electric potential concepts, and anyone seeking a deeper understanding of charge behavior in conductive materials.

yarospo
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This is a general question:

What is the electric potential of a hollow neutral conducting sphere with radius R with a charge q placed inside it?
Intuitively I understand that it is the same - q/R, no matter where the charge is placed inside the sphere. Can anyone explain why it is so?

My thoughts: The potential on the surface of a conducting sphere is constant, and it seems implausible that I will be able to change the potential of the sphere just by moving the charge inside, and therefore, I may as well place it in the middle and then the potential is obviously q/R.
 
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Hint: What would you expect the charge distribution to "look like" when you are very far from the sphere? What is the total charge enclosed by a spherical, concentric Gaussian surface of radius r>>R? So, if the potential at r=infinity is zero, what must the potential be at any point outside the sphere?
 
Thanks,

I've found a comprehensive and detailed explanation in Griffiths Intro to Electrodynamics. Should have known it'll be there - got to love that book!
:)
 

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