Electric Potential of Two Spherical Shells: Gaussian Surface Homework

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Homework Help Overview

The discussion revolves around the electric potential of two concentric spherical shells with given charges. The smaller shell has a positive charge, while the larger shell has a negative charge. Participants are exploring the electric potential at various distances from the center of the shells, specifically at points inside and outside the shells.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss calculating the electric potential at different distances, questioning the application of formulas and the interpretation of results. There is an exploration of the potential difference between the surfaces of the two shells and the use of Gaussian surfaces to analyze the charge enclosed.

Discussion Status

Some participants have provided guidance on how to approach the calculations for potential at various points, while others express confusion about the results and the application of concepts like Gaussian surfaces. There is an ongoing exploration of the implications of charge distribution and potential differences.

Contextual Notes

Participants are working under the constraints of homework guidelines, which may limit the information shared and the methods discussed. There are indications of uncertainty regarding the correct application of formulas and the interpretation of potential values.

rsatchel
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Homework Statement


A thin spherical shell with radius R1 = 2.00 cm is concentric with a larger thin spherical shell with radius 6.00 cm . Both shells are made of insulating material. The smaller shell has charge q1=+6.00nC distributed uniformly over its surface, and the larger shell has charge q2=−9.00nC distributed uniformly over its surface. Take the electric potential to be zero at an infinite distance from both shells.

Part A: What is the electric potential due to the two shells at the following distance from their common center: r = 0?
Part B: What is the electric potential due to the two shells at the following distance from their common center: r = 3.00 cm ?
Part C: What is the electric potential due to the two shells at the following distance from their common center: r = 7.00 cm ?

Homework Equations


V = ∫E. dl = (k q) / r
Φ = q(enc) / ε0 = ∫E.dA

The Attempt at a Solution


I got Part A:
V for inner shell: V= (k q) / r = (8.99E9 * 6.00E-9) / 0.02 = 2700
V for outer shell: V = (k q) / r = (8.99E9 * -9.00E-9) / 0.06 = -1350
ΣV = 2700 + (-1350) = 1350V

I eventually got Part B:
V = -k q1 (1/0.03 - 1/0.02) = 899V
V = -k q2 (1/0.06 - 1/ 0.03) = -1350
ΣV = 899 - 1350 = -450V (Although the answer had to be changed to +450, not really sure why...Maybe V is magnitude)

I tried doing the same thing Idid for Part B for Part C and got stuck:
V = -k q1 (1/0.07 - 1/0.02) = 1930V
V = -k q2 (1/0.07 - 1/ 0.06) = -192V
ΣV = 1930 - 192 = 1740V, but that is apparently wrong...

I'm thoroughly confused :/

 
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Hi rsatchel, Welcome to Physics Forums.

For part B, the location of interest lies between the shells. So it has the potential of the outer shell's surface plus whatever potential it experiences from the inner shell at its distance from that shell.

For part C, the location is outside of both shells so the easiest approach is to draw a Gaussian surface at the same radius and apply Gauss' Law. What's the total charge contained within the Gaussian surface?
 
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Ah, OK.
So I did q(net) = -3nC
V = (k q)( 1/inf - 1/0.07)
V = -(8.99E9 * -3E-9)(-1/0.007) = -385V
 
Ok, so now there's another part

What is the magnitude of the potential difference between the surfaces of the two shells?

I thought I would need to use:
V = ∫ E. dl = ∫ -(k q)/r dr (from A to B)
V = (-k q) / r again,
V = -k q( 1/B - 1/A)
but what would the limits be?

I thought maybe I should draw a Gaussian Surface at r=7cm and use the net charge to calculate the outer shell's potential and then do the same for the inner shell - didnt work.
I also tried doing the limits from the inner shell to the outer shell - didnt work.

Not sure what else to try :/
 
The potential at the surface of the outer shell will be due the total charge enclosed in a Gaussian surface immediately surrounding that shell.

The potential at the surface of the inner shell will be the potential due to that shell alone at its surface plus the potential due to the outer shell alone at that shell's surface (in passing into the interior space within the outer shell, the potential due to that outer shell is "remembered").

Have a look here for more details.
 
Thank you, that helped a lot!
 
gneill said:
The potential at the surface of the outer shell will be due the total charge enclosed in a Gaussian surface immediately surrounding that shell.

The potential at the surface of the inner shell will be the potential due to that shell alone at its surface plus the potential due to the outer shell alone at that shell's surface (in passing into the interior space within the outer shell, the potential due to that outer shell is "remembered").

Have a look here for more details.
hi could you make this link appear again "Have a look here for more details.[/QUOTE]"
 
SAADi_ak said:
hi could you make this link appear again "Have a look here for more details."
Unfortunately, website content often seems to "evaporate" over time. Alas that's not a website that I have any control over.

However, if you do a google search on appropriate terms you should be able to turn up similar content. Try searching on: "electric potential difference between charged concentric metallic shells".
 

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