Electric potential at the center of a insulating sphere

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Homework Help Overview

The discussion revolves around calculating the electric potential at the center of a uniformly charged insulating sphere with a specified radius and total charge. The problem involves understanding the relationship between electric field and potential, particularly in the context of integrating contributions from concentric spherical shells.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants explore the use of integrals to calculate electric potential and question the setup of limits of integration. Some suggest using the property of spherical shells contributing constant potential, while others express confusion over the signs in their calculations.

Discussion Status

The discussion is ongoing, with participants providing insights into potential approaches and clarifying concepts related to electric potential. There is acknowledgment of errors in setup and limits of integration, leading to differing signs in results. Some participants express a willingness to share methods if certain conditions are met.

Contextual Notes

Participants are working under the constraints of homework rules, which may limit the information they can share or the methods they can use. There is a focus on ensuring that the electric potential is calculated correctly, considering the conventions for potential at infinity.

SpringWater
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Homework Statement



Consider a uniformly charged insulating sphere with radius R and total charge Q in- side the sphere.

If Q = 2.9 × 10−6 C, what is the magnitude of the electric field at r=R/2 K=columbs constant. The answer to this question is E=(K)(Q) / (2)*(R)^(2)

The second part of the question which I am having trouble with is...

If the sphere has a radius of 3.3 m, find the potential at r = 0. The Coulomb constant is 8.98764 × 109 N · m2/C2 . Follow the convention that the electric potential at r = ∞ is zero. answer in units of V

Homework Equations


Q=2.9E-6 C
r=3.3m
k=8.98764E9 N*m^2 / C^2


The Attempt at a Solution



So I have set up the problem as two integrals

that are shown in the picture. I thought that this would give me the electric potential at r=0 however i am still getting it incorrect. I am not sure what I am doing wrong any help would be appreciated.
Thank you,
 

Attachments

  • hw7 #12.jpg
    hw7 #12.jpg
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Have you tried using the fact that the potential inside a spherical shell is constant and is equal to the potential on its surface?
 
Sunil Simha said:
Have you tried using the fact that the potential inside a spherical shell is constant and is equal to the potential on its surface?


I understood that concept but i guess because this was a two part problem i was trying to incorporate an integral that would relate to the first part of the problem, so no i really didnt...

..in that case the electric potential on the surface would be = (K)*(Q) / (R) Correct?

where R is the radius of the sphere and R=3.3 m
 
SpringWater said:
I understood that concept but i guess because this was a two part problem i was trying to incorporate an integral that would relate to the first part of the problem, so no i really didnt...

..in that case the electric potential on the surface would be = (K)*(Q) / (R) Correct?

where R is the radius of the sphere and R=3.3 m

no this is incorrect, so looking back at my integral, i am more sure that my set up was correct, in the orignal post w/ picture. the question now i believe is the sign (-) or (+)?
 
The second part can be solved by assuming the sphere to be made of thin concentric spherical shell of uniform charge densities. Every shell contributes a potential equal to that on it's surface. The solution is simply obtained by integrating the potentials. Note that Q is evenly distributed throughout the sphere and hence it helps to assign a constant as charge density and then use it.
 
Last edited:
Sunil Simha said:
The second part can be solved by assuming the sphere to be made of thin concentric spherical shell of uniform charge densities. Every shell contributes a potential equal to that on it's surface. The solution is simply obtained by integrating the potentials.

okay, thank you for the reply i greatly appreciate it.

using the integrals i set up, after simplifying the two i obtain -((3)*(k)*(Q) / (2)*(R)) which is a similar formula i just found a min ago however there formula did not have a negative sign. so why when my method is correct, do i come up with a negative sign assuming that the integral sums up the shells.
 
I'm a bit confused about how you got your limits of integration. Would you mind explaining? What is the final answer to this problem, by the way?
 
Averki said:
I'm a bit confused about how you got your limits of integration. Would you mind explaining? What is the final answer to this problem, by the way?


well i set them up incorrectly that is why i kept coming up with a negative answer. see picture for how i switched them. the worked integral is in the first attached picture however the answer should be positive.
 
Last edited:
Is the answer 3Q/8πεR? If correct I'll explain my method, else I'll check what I've done wrong and later suggest a solution.
 
  • #10
SpringWater said:
well i set them up incorrectly that is why i kept coming up with a negative answer. see picture for how i switched them. the worked integral is in the first attached picture however the answer should be positive.

sorry i forgot the picture.
 

Attachments

  • number 12 part two hw 7.jpg
    number 12 part two hw 7.jpg
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  • #11
Sunil Simha said:
Is the answer [itex]\frac{3Q}{8πεR}[/itex]. If correct I'll explain my method, else I'll check what I've done wrong and later suggest a solution.

yes, i get the same answer from your (simplified) solution and the same from the two integrals i set up however my problem was i did not set up the limits of integration correctly hence the negative sign.

thank you for your help
 

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