Understanding Part (b) of a Charge Distribution Problem

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Homework Help Overview

The discussion revolves around a charge distribution problem, specifically focusing on understanding part (b) of the question. Participants are analyzing electric field equations and potential energy calculations related to a given charge density.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Some participants discuss the electric field equations for different regions (r < a and r ≥ a) and express confusion regarding discrepancies in coefficients and variables used in the problem statement.
  • Participants question the assumptions made about the charge density and the implications of typesetting errors in the problem description.
  • There are inquiries about the integration process for potential and how it relates to the electric field derived from it.

Discussion Status

The discussion is ongoing, with participants offering insights into potential errors in the original poster's understanding and calculations. There is a recognition of the need for clarity regarding variable definitions and typesetting, but no consensus has been reached on the correct approach to part (b).

Contextual Notes

Participants note potential confusion arising from the use of different symbols (a vs. R) in the problem statement, which may affect the interpretation of the charge density. There is also mention of the importance of maintaining clarity in the original post to avoid further confusion in the discussion.

L_ucifer
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Homework Statement
A solid, nonconducting sphere of radius a has a volume charge density given by the equation ρ(r) = ρ0(r/a)^3, where r is the distance from the sphere’s centre.
(a) Determine the electric field magnitude, E(r), as a function of r.
(b) Determine the potential, V(r), as a function of r. Take the zero of potential at r = ∞.
Relevant Equations
E = -dV/dr
V = -W/q
I understand part (a) of this question, and my answer for that part is:

*For r < a*
E = (ρ0 * r4) / (6 * ε0 * a3)
* For r ≥ a*
E = (ρ0 * a3) / (6 * ε0 * r2)

Now, for part (b), I understand one solution is, for r < a, find the work done to bring a point charge q from infinity to a and then from a to r and divide the work by q. This solution is attached below:

Screenshot 2022-05-08 at 12.53.57 AM.png
Now, we also know that E = -dV/dr. This checks out because when we take the negative derivative of V found in the solution, we get the equation for E when r < a. This derivative can also be written as: V = -∫E*dr; however, when I integrate the equation of E for r < a, I get a different solution. Specifically, my solution is the same as the given solution except it doesn't have 6 as a coefficient for a2. Is there a gap in my understanding? What have I done wrong? I appreciate the support.

EDIT: Updated the variables and fixed the typesetting.
 
Last edited:
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L_ucifer said:
I understand part (a) of this question, and my answer for that part is:

*For r < a*
E = (ρ0 * r4) / (6 * ε0 * a3)
* For r ≥ a*
E = (ρ0 * R3) / (6 * ε0 * r2)
This does not seem correct to me. Please show your work.
 
Orodruin said:
This does not seem correct to me. Please show your work.
I apologise, I meant E = (ρ0 * a3) / (6 * ε0 * r2) for r ≥ a
Screenshot 2022-05-08 at 1.47.05 AM.png
Screenshot 2022-05-08 at 1.47.11 AM.png
 
Still incorrect with the problem as stated. You are not using the density quoted in the problem statement.
 
Orodruin said:
Still incorrect with the problem as stated. You are not using the density quoted in the problem statement.
I got the same fields as OP with ##\rho(r)=\rho_0\left(\dfrac{r}{a}\right)^3##. Maybe the discrepancy is due to careless typesetting in the statement of the problem in which the radius of the distribution appears ##R## instead of ##a##. The ratio ##r/a## is cubed in the solution, not multiplied by 3.
 
kuruman said:
I got the same fields as OP with ##\rho(r)=\rho_0\left(\dfrac{r}{a}\right)^3##. Maybe the discrepancy is due to careless typesetting in the statement of the problem in which the radius of the distribution appears ##R## instead of ##a##. The ratio ##r/a## is cubed in the solution, not multiplied by 3.
Yes, I am not sure why R and a have been switched, but the radius of the sphere is a.
 
L_ucifer said:
Yes, I am not sure why R and a have been switched, but the radius of the sphere is a.
Welcome to PF. Please learn to post using LaTeX here -- it makes it much easier to quote and edit your posts. See the "LaTeX Guide" link at the lower left of the Edit window. Thanks.
 
kuruman said:
I got the same fields as OP with ##\rho(r)=\rho_0\left(\dfrac{r}{a}\right)^3##. Maybe the discrepancy is due to careless typesetting in the statement of the problem in which the radius of the distribution appears ##R## instead of ##a##. The ratio ##r/a## is cubed in the solution, not multiplied by 3.
The exponent is not the issue. The issue is ##a## or ##R## appearing in the ratio in the OP (which OP has now edited) and subsequently in the solution.

@L_ucifer Please do not edit your OP after replies are in place. It only serves to confuse people who are coming into the thread what the previous posts are about. If you need to correct the statement, do so in a follow-up post.
 
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Orodruin said:
The exponent is not the issue. The issue is ##a## or ##R## appearing in the ratio in the OP (which OP has now edited) and subsequently in the solution.

@L_ucifer Please do not edit your OP after replies are in place. It only serves to confuse people who are coming into the thread what the previous posts are about. If you need to correct the statement, do so in a follow-up post.
Well, this has gone horrendously for me and I do apologise for these silly errors. You live you learn, I guess. Ignoring all my logistical errors, is there any solution to my question?
 
  • #10
Where in your solution for the potential for r<a do you not agree with the provided solution?
 

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