Charge distributions of two infinite parallel plates

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SUMMARY

The discussion focuses on the charge distribution of two infinite parallel conducting plates with excess charges of 2Q and 3Q. It is established that the surface charge densities are related through the equations σ1 = -σ2 and σ2 = -σ3, indicating that the electric field inside the plates is zero while the field between them is determined by the difference in surface charge densities. The magnitude of the electric field between the plates can be expressed as E = (σ1 - σ2)/(2ε₀), where ε₀ is the permittivity of free space.

PREREQUISITES
  • Understanding of Gauss's Law
  • Familiarity with electric fields and surface charge density
  • Knowledge of the properties of conductors in electrostatics
  • Basic mathematical skills for manipulating equations
NEXT STEPS
  • Study the derivation of electric fields from surface charge densities using Gauss's Law
  • Learn about the behavior of electric fields in the presence of conductors
  • Explore the concept of infinite charge distributions and their implications
  • Investigate the effects of varying charge distributions on electric field strength
USEFUL FOR

This discussion is beneficial for physics students, educators, and anyone interested in electrostatics, particularly those studying the behavior of electric fields between charged conductors.

MaximumTurtles
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Homework Statement


Two infinitely large conducting plates with excess charge 2Q and 3Q are placed parallel to one another, and at a small distance from one another. How are the charges 2Q and 3Q distributed? You may assume that infinitely large sheets of charge produce electric fields that are distance-independent. Make sure not to just guess or list the charge distribution, but to prove it! Based on your result, can you state the formula for the magnitude of the field between these two parallel very large conducting plates, as well as the formula for the field between any two parallel very large conducting plates?

Homework Equations


This is in a practice test for a chapter on Gauss's law.

The Attempt at a Solution


I have tried setting up two Gaussian surfaces, the first is a cylinder with one end inside each plate, the other with each end on the outside of each plate. I can relate the surface charge densities to the electric fields outside, and I can get the relationship between the inner surfaces, but I can't figure out how to get a relationship between the charges 2Q and 3Q (written as Q and Q' in my diagram) and the surface charge densities.

Here is my attempt:

https://drive.google.com/open?id=16OxjQOXjbZ0hBXws6ZkEGEu0gQ0aWe9t

This is my first time posting, so I apologize for being a noob, let me know if there's anything I can do to help out.
 
Last edited:
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Hello MaxT, :welcome:

A good starting post, but my neck hurts from craning sideways. You place Q and Q' in ambuiguous locations: it is known that positive charge repels positive charge, so for a single plate the charges would not stay in the bulk volume, but move (conductor!) to a suitable surface.
The exercise is a bit complicated by the repeated use of the term 'infinitely', but never mind (replace by 'very'). And: you do the right thing by switching to surface charge density.
I agree with σ1 =-σ2 [edit - now that I can see the subscripts] ##\ \sigma_2 = -\sigma_3\ ## but that's about all I can decipher.

Any other useful Gauss surfaces ? How should the total charge distribution behave when seen from 'infinitely' :smile: far away ? All field lines have which direction ?
 
Last edited:
BvU said:
A good starting post, but my neck hurts from craning sideways.

Haha, woops, I fixed that! Sorry about the wording of the question, the professor's English isn't too good, but I copied down what he wrote exactly. Practically speaking, he just want the plates to be large enough that we can consider the electric field they create to be distance-independent (E = sigma/(2*epsilon naught)).

I can see that the areas outside the plates will have a field strength equal to the sum of the fields created by all 4 surfaces, the inside of the plates will have a zero field, and the area in between will be the difference between the fields created by the top plate and the bottom plate. I still can't see how to get the surface charge densities in terms of the charges of the plates though.
 
Last edited:
Fixed my sigma subscript numbers. What do you know about ##\ \sigma_1+\sigma_2\ ## in relation to ##\ \sigma_3+\sigma_4\ ## ?
 
MaximumTurtles said:
the inside of the plates will have a zero field
what equations does that give you in terms of the four surface charge densities?
 

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