Calculating Potential Inside a Uniformly Charged Sphere

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Homework Help Overview

The discussion revolves around calculating the electric potential inside a uniformly charged sphere, with participants exploring the relationship between electric field and potential, as well as the implications of choosing reference points for potential.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to calculate the potential inside the sphere using the electric field and questions the validity of their approach, particularly regarding the choice of limits for integration and the reference potential. Other participants inquire about the electric field used and suggest clarifications on the integration process.

Discussion Status

Participants are actively engaging with the problem, providing feedback on the electric field and potential calculations. There is a recognition of the need to maintain consistency in reference points for potential, and some guidance has been offered regarding the integration limits and the application of Gauss' Law.

Contextual Notes

There is an ongoing discussion about the implications of setting the reference potential at infinity versus at the origin, and how this affects the calculations of potential inside and outside the sphere. Participants are also addressing the correct application of the electric field in different regions.

philipc
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I have a sphere of uniform charge density and I need to find the potential inside and outside. I found it for the outside, but I am wondering if my solution for the inside is correct. I used dV = E*dl,(* being the dot product) For my lower limit I used r, where r < a and "a" being the radius. For the upper limit I used zero because when r is zero, I figured zero potential because you have zero charge. The only problem I get a negative potential? Does this sound right?
Thank You
Philip
 
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What exactly did you use for the E field inside the sphere?
 
E = (p* r) / (3* e)
results
V = - (p r^2) / (6*e)

where p = roe and e = permittivity

Thanks
 
Your E field looks good.

Regarding the potential, since you didn't state it in your problem you are free to set the reference potential anywhere you want. Usually one takes the potential to be zero at infinity when dealing with a charge distribution of finite extent. However, once you choose your reference potential you must use it consistently throughout the analysis.

For example, if you set the potential equal to zero at infinity then the potential everywhere is relative to that. In that case you might perform your integration of the electric field starting at infinity and working inward. The potential at the origin will be relative to that. Similarly, you could set the potential at the origin to be zero in which case the potential at infinity will not be zero!

The sign or value of potential matters little since ultimately it is potential difference or gradient of the potential that matters.
 
OK I see what you are saying. I placed zero V at infinity when working outside sphere, so therefore I need to stick with the same. Let me make sure I have the concept down, I'm heading in from infinity and reach the out side of the sphere, this is where my V will be the greatest because my E is the greatest here right?
But if I was to intgrate from r to infinity, then infinity will be on the top and does not go to zero, my V does not look right this is what I get using r and infinity as my limits of intgration, p/(6*e) *(r^2-infinity), this doesn't see right?

Thanks again for you help
Philip
 
From Gauss' Law you know the electric field everywhere. You have to use the appropriate value of the electric field at every point along your path of integration. It looks like you're trying to use the analytic form of the electric field INSIDE the sphere EVERYWHERE! NO! For any and all points outside the sphere you use the 1/r^2 form and the r form applies ONLY inside. E.g. if you choose to integrate from infinity the integral corresponding to points INSIDE the sphere will look something like

[tex]\int_{\infty}^{R} \frac {1}{s^2} ds + \int_{R}^{r} s ds[/tex]
 
Ok that makes much more sense.
Thanks for your help
Philip
 

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