Method of Images: Infinite, charged wire above a grounded plate

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SUMMARY

The discussion focuses on solving the potential, V(x,y,z), above a grounded conducting sheet due to an infinitely long wire with charge density λ positioned at a distance d above the sheet. The method of images is employed by introducing an imaginary wire with charge density -λ located at -d below the sheet, effectively simplifying the problem. The potential of an infinitely long charged wire is expressed as φ = (-λ/2π) ln(r/a), where r is the distance from the wire and a is an arbitrary reference point. This approach is crucial for accurately determining the induced charge on the sheet and understanding the potential distribution in the vicinity of the wire.

PREREQUISITES
  • Understanding of electrostatics and potential theory
  • Familiarity with the method of images in electrostatics
  • Knowledge of logarithmic functions and their properties
  • Access to Griffiths' "Introduction to Electrodynamics" for reference
NEXT STEPS
  • Study the method of images in electrostatics for various geometries
  • Learn about the potential of charged wires and their implications in electrostatics
  • Explore problems involving multiple grounded planes and their interactions with line charges
  • Review Jackson's "Classical Electrodynamics" for advanced applications of the method of images
USEFUL FOR

Students and professionals in physics, particularly those studying electrostatics, electrical engineering, and anyone seeking to deepen their understanding of potential theory and the method of images.

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Homework Statement


Given an infinitely long wire, with charge density \lambda, parallel to and a distance d above an infinite, grounded, conducting sheet, what is the potential, V(x,y,z) above the sheet?

What is the induced charge on the sheet?


Homework Equations




The Attempt at a Solution



This is a method if images problem. Construct a infinitely long wire with charge density -\lambda a distance -d below the plane of the sheet and then disregard the sheet (it creates the same potential, V=0, at the plane of the sheet).

However, I ran into a snag when I tried to find the potential of an infinitely long charged wire. Is the potential infinite?
 
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No... if you have the Griffiths book please look at page 80. There is a very important discussion in there where students mostly pass reading it very fast!

Due to the argue in the last past of page 80, you can not choose the infinity as your potential reference point. you can choose it is a arbitrary point named a, for example so the potential of a infinite charged line will be:

(-lamda/ 2pi) Ln (r/a)

which r is the distance from the wire
 
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aha! Thanks astrosona. That's something I've forgotten about.
 
In fact, due to the properties of logarithms, you can rewrite this as

\phi = -\frac{\lambda}{4\pi} \ln \frac{r^2}{a^2}

which might make some things simpler to calculate, because r^2 = x^2 + y^2, and you no longer have to bother with square roots.

Your problem is pretty simple, but in Jackson's there is a similar problem with two grounded planes, meeting at right angles, with the line charge located at (x_0, y_0). :P
 

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