Concepts regarding Electric Potentials of Spheres

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Homework Help Overview

The discussion revolves around understanding electric potentials related to spheres, particularly focusing on the behavior of potential inside and outside conducting and non-conducting spheres. Participants are exploring concepts of electric fields, potential differences, and the implications of charge distribution.

Discussion Character

  • Conceptual clarification, Assumption checking, Exploratory

Approaches and Questions Raised

  • Participants discuss the implications of charge distribution on electric potential, questioning the behavior of potential inside hollow and solid spheres. There are attempts to clarify the conditions under which potential remains constant and the relationship between electric fields and potential differences.

Discussion Status

Some participants are actively clarifying their understanding of electric fields in relation to charge presence, while others are confirming the correctness of their reasoning regarding potential differences. There is an ongoing exploration of concepts without a clear consensus yet.

Contextual Notes

Participants are navigating assumptions about charge distribution and the nature of electric fields in different geometries, with references to external sources for further clarification. The discussion reflects a mix of established principles and personal interpretations that may require further examination.

WWCY
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Homework Statement


Screen Shot 2017-03-01 at 2.59.42 PM.png

My questions are just related to part a of this problem.

Homework Equations

The Attempt at a Solution


I know that potential inside a conductor is equivalent to potential on the surface of the conductor and potential at any point is an algebraic sum of potential contributions from surrounding sources. But this is as far as I got..

I gathered that potential on surface of b is 0, as net charge of the sphere is 0 (after treating both spheres as point charges of +q and -q). By my previous statement, shouldn't potential inside sphere b (for example r_a < r < r_b) 0 as well?

Could anyone point out the gaps in my understanding? Any help is very much appreciated.
 
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WWCY said:
shouldn't potential inside sphere b (for example r_a < r < r_b) 0 as well
That's not a conducting volume !
 
BvU said:
That's not a conducting volume !

So...
a) Potential is only constant across solid conducting objects?
b) How do I deduce the Potential inside a hollow sphere? Does the Vab = ∫ E . dr still come into play?

Thank you

edit:
This source seems to state that there isn't any voltage difference between the surface of the shell and its interior though, what am I missing?
http://www.phys.uri.edu/gerhard/PHY204/tsl93.pdf
 
Here's another stab at the problem.
I tried to be as detailed as possible in explaining my steps and thought processes... Does this look right? Thank you!

1488434887714.jpg
 
Can't read any of that.
How do you determine the potential from the inner sphere if the outer would not be there at all ?
 
BvU said:
Can't read any of that.
How do you determine the potential from the inner sphere if the outer would not be there at all ?

Oops, apologies.

The potential from the inner sphere is as if it originates from a point charge so... v = kq/r? for r>ra
 
Bingo. But: do you realize you now are ready with the exercise ?
 
BvU said:
Bingo. But: do you realize you now are ready with the exercise ?

Yeah, i believe i do. Might I clarify a few concepts?

1) My initial assumption that field in a hollow sphere should be 0 is wrong because that was based on the assumption that there was no charge enclosed in it, yes? Since there is now a +q in the hollow space, there exists an E-field, which also means that there is a potential difference between points in the hollow space and the surface of the hollow sphere. i.e. for r where ra < r < rb, therefore V =/= 0 for points in the hollow space.

2) There is no field in the small solid sphere because there is no charge in it. Therefore there is no E-field and no potential difference between points in the sphere "a" and on the surface of that sphere.

So taking Va to be potential for points in the smaller solid sphere, and using Va - Vb = ∫ E . dr and then splitting the integral limits into:
1) r<ra to ra - where field is 0
2) ra to rb - field present
3) rb to ∞ - field and potential = 0 (this means Vb = 0)

should see me obtain the potential of points in the smaller sphere, is this right?

Again, apologies if I'm not getting my points across as clearly as i should be. Thanks for your patience.
 
WWCY said:
1) My initial assumption that field in a hollow sphere should be 0 is wrong because that was based on the assumption that there was no charge enclosed in it, yes?
Correct.
Since there is now a +q in the hollow space, there exists an E-field, which also means that there is a potential difference between points in the hollow space and the surface of the hollow sphere. i.e. for r where ra < r < rb, therefore V =/= 0 for points in the hollow space.
Correct again
2) There is no field in the small solid sphere because there is no charge in it.
In the sense that all the charge sits on the surface, yes.
Therefore there is no E-field
In a conductor there is no E-field because if there were, the charges would move (after all, it's a conductor!) until there is no more E-field
and no potential difference between points in the sphere "a" and on the surface of that sphere.
Right.
WWCY said:
should see me obtain the potential of points in the smaller sphere, is this right?
Right again.
WWCY said:
Again, apologies if I'm not getting my points across as clearly as i should be. Thanks for your patience.
No need to apologize. And: you're welcome.
 

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