Potential difference in uniformly charged cylinder

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SUMMARY

The discussion focuses on calculating the potential difference between the surface and the axis of a uniformly charged cylinder with charge density ρ and radius R. The correct approach involves using a cylindrical Gaussian surface, leading to the electric field E = ρ / (2πRε₀). The potential difference is then derived as ΔV = - (ρ / (2πε₀)) ln(R). This method effectively parallels the approach used for an infinite line of charge, confirming its validity.

PREREQUISITES
  • Understanding of Gaussian surfaces in electrostatics
  • Familiarity with electric field calculations for charged objects
  • Knowledge of potential difference and its mathematical representation
  • Proficiency in calculus, particularly integration techniques
NEXT STEPS
  • Study the derivation of electric fields using Gaussian surfaces
  • Learn about potential difference calculations in electrostatics
  • Explore the properties of uniformly charged cylinders and their electric fields
  • Investigate the relationship between electric fields and potential for various charge distributions
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Students of electromagnetism, physics educators, and anyone involved in electrostatics calculations will benefit from this discussion.

Alexander2357
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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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