Solving Gauss's Law Problem for Electric Field

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Homework Help Overview

The problem involves applying Gauss's Law to determine the electric field and potential in various regions surrounding a uniformly charged ball and a hollow metal shell. The context is centered around electrostatics and electric fields.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to express the electric field in terms of the charge density and questions whether to eliminate the volume charge density from their calculations. Some participants suggest expressing the answer in terms of the given variables.

Discussion Status

Participants are exploring different aspects of the problem, including the relationship between charge density and total charge. There is an ongoing discussion about the potential in various regions, with some participants sharing their calculations and seeking confirmation of their results.

Contextual Notes

The original poster mentions additional parts to the problem, including finding potentials in specified regions and sketching graphs of electric field and potential as functions of distance from the center of the sphere. There is also a request for assistance in posting graphs without a scanner.

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Homework Statement


A uniformly charged ball of radius a and a total charge -Q is at the center of a hollow metal shell with inner radius b and outer radius c. The hollow sphere has a net charge +2Q. Find the magnitude of the electric field in the regions: r_1 < a,a < r_2 < b,b < r_3 < c, and r_4 > c.

Homework Equations



V = \frac{4}{3} \pi R^3
S = 4 \pi R^2
\oint E(x)dA = \frac{q_{in}}{\epsilon_o}

The Attempt at a Solution



For E(r1 < a):
\rho = \frac{Q_{tot}}{\epsilon_o}
Q_{in,tot} = \rho*\frac{4}{3} \pi r_1^3
\oint_0^rE(x)dA = \frac{q_{in}}{\epsilon_o}

E(r_1) = \frac{\rho\frac{4}{3} \pi r_1^3}{\epsilon*4 \pi r_1^2}

E(r_1) = \frac{\rho*r_1}{3\epsilon_o}

This is actually where I am stuck, I got everything else. Am I supposed to get rid of that volume charge density, \rho?
 
Last edited:
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Yes; in textbook problems, they expect you to express the answer in terms of the variables given in the statement of the problem.

The density is uniform and you know the total charge in the little ball. So just divide that by its volume to find its density.
 
The following may help.

Regards,

Nacer.

http://islam.moved.in/tmp/c.jpg
 
Last edited by a moderator:
There is actually a second and third part to this question:

b) Find potentials at points in the regions: r_1 &lt; a, a &lt; r_2 &lt; b, b &lt; r_3 &lt; c, and r_4 &gt;c

For r1 < a,
I use the formula

V_o - V_{r_1} = \int_0^r E(r_1)dr

E(r_1) = \frac{\rho*r_1}{3\epsilon_o}

V_o - V_{r_1} = \frac{\rho}{3\epsilon_o} \int_0^r r dr

V_o - V_{r_1} = \frac{\rho*r_1^2}{6\epsilon_o}

Solving the same way, I got::

V_o - V_{r_2} = \frac{Q}{4 \pi \epsilon_o r_2}

V_o - V_{r_3} = 0

V_o - V_{r_4} = \frac{-Q}{4 \pi \epsilon_o r_4}

Did anyone get the same answer as I did?

Also, I am supposed to sketch the graphs of how Ex depends on a distance(r) from the center of the sphere, and how V depends on a distance(r) from the center of the sphere.

I drew my graphs, but I don't know how to post it on. I don't have a scanner handy, so if anyone can help, please let me know what your graphs looks like.
Thank you very much, you are all so helpful.
 

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