Electric field between two metal plates

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Homework Help Overview

The discussion revolves around the electric field between two large, flat metal plates that are oppositely charged. The problem involves applying Gauss's law to determine the electric field inside and outside the plates, as well as considering the implications of using non-conductors instead of conductors.

Discussion Character

  • Conceptual clarification, Assumption checking, Exploratory

Approaches and Questions Raised

  • The original poster attempts to apply Gauss's law to derive the electric field between the plates and questions how the results would differ if the plates were non-conductors. Participants discuss the implications of charge distribution in conductors versus non-conductors and the conditions for static equilibrium.

Discussion Status

Participants are exploring the differences between conductors and non-conductors, with some providing hints and asking clarifying questions. There is an ongoing examination of assumptions made in the original poster's approach, particularly regarding charge distribution and electric field behavior.

Contextual Notes

Participants note the importance of understanding the conditions that apply specifically to conductors, such as the behavior of electric fields within and outside the plates, and the implications of static equilibrium in the context of charge distribution.

toothpaste666
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Homework Statement


Two large, flat metal plates are separated by a distance that is very small compared to their height and width. The conductors are given equal but opposite uniform surface charge densities +σ and -σ. Ignore edge effects and use Gauss's law to show
a) the electric field between the plates
b) the electric field on on the outside of the plates on either side
c) how would my results be altered if the two plates were non conductors

Homework Equations


∫EdA = Q/ε

The Attempt at a Solution


a)
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I made a imaginary cylinder where the surface A is perpendicular to the electric field
∫EdA = Q/ε
the Q enclosed is going to be the charge density times the area enclosed or σA
∫EdA = EA = σA/ε
the As cancel so
E = σ/ε

b) picture the same imaginary cylinder but fully extending all the way through and out the other side of both conductors now the Q on the right hand side of gauss's equation is the net sum of the enclosed charge or
Q = σA+ -σA = 0 so E = 0

c) this part I can't figure out. i need a hint to get started =[
 

Attachments

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Hint:

1. What's the difference of conductor and non-conductor?

2. Ask yourself what the meaning of every step in (a) and (b) is.

You know there's something different in calculation when you are dealing with non-conductors.
However, you didn't find those "key condition" which is only fit with conductor.
 
Last edited:
a non conductor will have no net charge?
 
also since they are conductors does that mean the left surface of the positive plate will have a negative charge?
 
1. For (a), you assume the electric field inside the plate is zero, and that's different in non-conductor case.

2. For (a), you assume the electric field outside the plate is perpendicular to the surface of metal plate, that's also different in non-conductor case.

toothpaste666 said:
also since they are conductors does that mean the left surface of the positive plate will have a negative charge?

I'm not sure why you think the left surface of the positive plate will have a negative charge in conductor case. But I think if there's still a negative charge in positive plate, then that means the positive plate is not in equilibrium state: static electricity equilibrium.

Suppose that there's a conductor and has positive charge on the one side and negative charge in the other side. Then, there must be some electric lines between the positive and negative charges( just like what you said). That means, those "hidden free electron" will be influenced by the electric field inside the conductor and starts moving until the electric field inside the conductor is zero, i.e. it's in static electricity equilibrium.
 

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