Spherical Shells and Gauss' Law

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Homework Help Overview

The problem involves calculating the electric field in the context of two concentric insulating spherical shells with given charge distributions. The inner shell has a total charge q, while the outer shell has a charge of -q. The discussion focuses on determining the electric field in different regions defined by the radii of the shells.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the application of Gauss' Law to find the electric field in specified regions. There are attempts to derive expressions for the electric field in the regions between the shells and questions about the direction of the electric field. Some participants express uncertainty about the contributions of the charges from both shells, particularly in the outer region.

Discussion Status

There is ongoing exploration of the electric field expressions for each region, with some participants confirming the correctness of certain derived equations. Questions remain regarding the proper summation of electric fields from both shells and the direction of the field in specific regions. Guidance has been offered regarding the contributions of the charges and the overall direction of the electric field.

Contextual Notes

Participants are working under the constraints of homework guidelines, which may limit the information provided. There is a focus on ensuring that the assumptions about charge distributions and their effects on the electric field are clearly understood.

Soaring Crane
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Homework Statement



A small, insulating, spherical shell with inner radius a and outer radius b is concentric with a larger insulating spherical shell with inner radius c and outer radius d. The inner shell has total charge q distributed uniformly over its volume, and the outer shell has charge -q distributed uniformly over its volume.

http://i131.photobucket.com/albums/p289/SoaringCrane/yf_Figure_22_391.jpg

Calculate the magnitude of the electric field and direction of the field (outward or toward the center) for

i. a < r < b
ii. b < r < c
iii. c < r < d


Homework Equations



See below.

The Attempt at a Solution


--------------------------------------------------------------------------
General workings for shell with inner radius a and outer radius b:

Q = rho*(4/3)*pi[b^3 – a^3], where Q = total uniform charge

indefinite integral[E*dA] = q_enclosed/epsilon_0

E*4*pi*r^2 = [rho*(4/3)*pi[r^3 – a^3]]/[epsilon_0]
--------------------------------------------------------------------------

Note that then rho for inner shell = q/[(4/3)*pi*(b^3-a^3)] and outer shell rho = [-q]/[(4/3)*pi*(d^3-c^3)] in this specific problem.

a. E = [q/(4*pi*epsilon_0)]*[(r^3 – a^3)/(b^3-a^3)]*(1/r^2)

The direction will be away from the center??

b. Total charge is q, so E = (1/4*pi*epsilon_0)*(q/r^2) This will be outward the center, too?

c. This one I am really unsure of—both with the direction and electric field expression since two different charges are featured.
At first, I thought it would be [-q*(r^3 – d^3)]/[4*pi*epsilon*r^2*(c^3 – d^3)], but this alone is wrong?

Would it be a sum:

[-q*(r^3 – d^3)]/[4*pi*epsilon*r^2*(c^3 – d^3)] + [q/(4*pi*epsilon_0)]*[(r^3 – a^3)/(b^3-a^3)]*(1/r^2) + (1/4*pi*epsilon_0)*(q/r^2) ?

As for direction, would it be outward, too? A positive test charge would move away from the positively charged shell and move towards the negative shell?

Any help is appreciated. Thank you.
 
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Can anyone please help me with part iii. and check my direction answers for the other parts?

Thank you again.
 
Soaring Crane said:
a. E = [q/(4*pi*epsilon_0)]*[(r^3 – a^3)/(b^3-a^3)]*(1/r^2)

The direction will be away from the center??

b. Total charge is q, so E = (1/4*pi*epsilon_0)*(q/r^2) This will be outward the center, too?
These look OK to me.

c. This one I am really unsure of—both with the direction and electric field expression since two different charges are featured.
At first, I thought it would be [-q*(r^3 – d^3)]/[4*pi*epsilon*r^2*(c^3 – d^3)], but this alone is wrong?
Here it seems like you just considered the outer shell of charge but forgot to include the inner shell.

Would it be a sum:

[-q*(r^3 – d^3)]/[4*pi*epsilon*r^2*(c^3 – d^3)] + [q/(4*pi*epsilon_0)]*[(r^3 – a^3)/(b^3-a^3)]*(1/r^2) + (1/4*pi*epsilon_0)*(q/r^2) ?
It would be the sum of the field from the partial outer shell plus the field from the total inner shell--you've computed them both, just add them up.

As for direction, would it be outward, too? A positive test charge would move away from the positively charged shell and move towards the negative shell?
The field at point r just depends on the total charge within the spherical surface at r. In this problem, that total charge is always positive for all points up to r = d, thus it points outward at all points.
 
The sum will be:


total inner shell, (1/4*pi*epsilon_0)*(q/r^2), + partial outer shell,
[-q*(r^3 – d^3)]/[4*pi*epsilon*r^2*(c^3 – d^3)] ?

Or did I use/mismatch the wrong expressions?
 
That looks good to me.
 

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