EM Problem: Floating Conducting Cylinder

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SUMMARY

The discussion centers on solving the electromagnetic problem of a floating conducting cylinder using image theory and Laplace's equation in cylindrical coordinates. The initial approach involved Gauss's law, which proved inadequate due to the non-uniform charge distribution. The professor recommended using image theory to simplify the problem by introducing an imaginary conductor of opposite charge beneath the ground plane. The goal is to determine the capacitance between the cylinder and its image, which is crucial for understanding the electric field distribution.

PREREQUISITES
  • Understanding of Gauss's law and its limitations in non-uniform charge distributions
  • Familiarity with image theory in electrostatics
  • Knowledge of Laplace's equation in cylindrical coordinates
  • Basic concepts of capacitance and electric field distribution
NEXT STEPS
  • Study the application of image theory in electrostatics problems
  • Learn how to solve Laplace's equation in cylindrical coordinates
  • Research capacitance calculations for cylindrical conductors
  • Review advanced electromagnetism texts, such as "Classical Electrodynamics" by Jackson
USEFUL FOR

This discussion is beneficial for physics students, electrical engineers, and anyone involved in solving complex electromagnetic problems, particularly those related to electrostatics and capacitance.

jegues
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Homework Statement



See figure attached.

Homework Equations





The Attempt at a Solution



Originally I have solved this problem using Gauss's law by defining a gaussian surface in the form of a cylinder around the floating cylinder to get the electric field distribution underneath the cylinder to ground.

The result I obtained was,

V(y) = \frac{Q_{pul}}{4 \pi \epsilon_{0}}\left( \frac{ln(d-y)}{d} \right)

but since we aren't told what Qpul is we cannot plot the variation of the voltage.

My professor suggested I try solving this problem using image theory and laplaces equation in cylindrical coordinates in order to avoid Qpul.

Can someone explain to me how this done?

Thanks again!
 

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jegues said:
My professor suggested I try solving this problem using image theory and laplaces equation in cylindrical coordinates in order to avoid Qpul.

Can someone explain to me how this done?

Thanks again![/QUOTE

Problem with Gaussian surface is, the charge is not uniformly distributed so you can't take advantage of symmetries.

The image is a similar conductor of opposite sign a distance d below the ground.

This is a real bear of a problem. What you want is the capacitance between the cylinder and the conducting plane, i.e. the capacitance between the cylinder and its image.

Do you use Jackson?
 

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