Potential difference in uniformly charged cylinder

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Homework Help Overview

The problem involves finding the potential difference between the surface and the axis of a uniformly charged cylinder with a specified charge density ρ. The context is rooted in electrostatics, specifically dealing with electric fields and potential differences in cylindrical geometries.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the choice of Gaussian surfaces, debating between using a cylinder or a sphere for calculating the electric field. Questions arise about the implications of using an infinite area and how to handle the charge distribution within the chosen surface.

Discussion Status

Some participants have offered insights into the electric field due to an infinite line of charge and suggested applying similar reasoning to the cylinder. There is an ongoing exploration of different approaches, with some participants expressing uncertainty about their calculations and seeking validation of their results.

Contextual Notes

Participants note the challenge of determining the appropriate Gaussian surface and the implications of the infinite nature of the cylinder. There is a mention of previous experiences with related problems, indicating a shared context for understanding the current issue.

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Homework Statement



Charge is uniformly distributed with charge density ρ inside a very long cylinder of radius R.

Find the potential difference between the surface and the axis of the cylinder.

Express your answer in terms of the variables ρ, R, and appropriate constants.

Homework Equations



\int \overrightarrow{E}.d\overrightarrow{A}=\frac{Q }{\epsilon _{0}}

\Delta V = -\int_{i}^{f}\overrightarrow{E}.d\overrightarrow{s}

The Attempt at a Solution



I am struggling with determining which Gaussian surface to use. If I use a cylinder, then the cylinder would have an infinite area, right? How can I deal with that? If I use a sphere (since I am trying to find the potential difference between only two points, one on the surface and one on the axis), what will be the charge inside the sphere?

If I use a sphere as my Gaussian surface, I get:

E = \frac{\rho }{4\pi R^{2}\epsilon _{0}}

\Delta V = \frac{\rho }{4\pi R^{2}\epsilon _{0}} \int_{0}^{R}dR=\frac{\rho }{4\pi R\epsilon _{0}}

But this is wrong.

If I use a cylinder as my Gaussian surface instead, I get the following, but it doesn't look right:

\Delta V = \frac{\rho }{2\pi \epsilon_{0}}\int_{0}^{R}\frac{1}{R} dR
 
Last edited:
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I am struggling with determining which Gaussian surface to use. If I use a cylinder, then the cylinder would have an infinite area, right? How can I deal with that?
It's like when you find the field due to an infinite line of charge. Have you done that one (or had it done for you)?
 
Simon Bridge said:
It's like when you find the field due to an infinite line of charge. Have you done that one (or had it done for you)?

Yes, I did that a few weeks ago.

The electric field due to an infinite (very long) line of charge is:

\frac{\rho }{2\pi R \epsilon_{0}}

If I substitute this into the equation for potential difference, I get:

\Delta V = -\frac{\rho }{2\pi \epsilon_{0}}ln(R)

Is this correct?
 
My point is - why not try the same shape gaussian surface as for the long line of charge?
 
Simon Bridge said:
My point is - why not try the same shape gaussian surface as for the long line of charge?

Thank you for your help Simon. I managed to get the right answer.
 
Well done.
 

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