Find the magnitude of the electric field at regions 2 and 3.

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Homework Help Overview

The problem involves calculating the electric field at specific regions created by three parallel planes of charge with varying surface charge densities. The context is rooted in electrostatics and the behavior of electric fields due to charged planes.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the electric field behavior in regions 1, 2, 3, and 4, noting that the fields in regions 1 and 4 are zero. Questions arise regarding the logic used to determine these values and how it applies to regions 2 and 3.

Discussion Status

There is an ongoing exploration of the reasoning behind the electric field calculations. Some participants have offered clarifications regarding the electric field due to infinite planes of charge, while others are questioning the assumptions made about the fields in different regions.

Contextual Notes

Participants are grappling with the definitions and properties of electric fields from charged planes, and there is a noted confusion between the electric fields of infinite planes and conductors in electrostatic equilibrium. This indicates a potential gap in understanding that is being addressed through discussion.

Mason Smith
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Homework Statement


The three parallel planes of charge shown in the figure have surface charge densities (-1/2)η, η, and (-1/2)η.

24.45.JPG


Homework Equations


I think that the electric field is equal to eta divided by epsilon naught.

The Attempt at a Solution


Well, I know that the electric field at regions 1 and 4 are zero.
E1 = E4 = (-1/2)η + η + (-1/2)η = 0.
I know that the electric field in region 2 points upward and that the electric field at region 3 points downward. However, I am not sure how to calculate the electric field in these regions. How do I go about calculating the electric field in these regions?
 
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Mason Smith said:

Homework Equations


I think that the electric field is equal to eta divided by epsilon naught.
Check your notes. The field due to a single infinite plane of charge density ##\eta## is not ##\frac{\eta}{\epsilon_0}##.

The Attempt at a Solution


Well, I know that the electric field at regions 1 and 4 are zero.
How do you know that? The reason I ask this question is that the logic for deducing that the field is zero in regions 1 and 4 is similar to the logic for finding the fields in regions 2 and 3.
 
TSny said:
Check your notes. The field due to a single infinite plane of charge density ##\eta## is not ##\frac{\eta}{\epsilon_0}##.How do you know that? The reason I ask this question is that the logic for deducing that the field is zero in regions 1 and 4 is similar to the logic for finding the fields in regions 2 and 3.
Oh, yes. I confused the electric field for an infinite plane of charge with the electric field of a conductor in electrostatic equilibrium.
Well, when I worked the problem by saying that E4 = E1, I got an answer of zero. I put that answer into MasteringPhysics. The answer was correct. Using that same reasoning with the electric field in regions 2 and 3 proved wrong.
 
Well, when I worked the problem by saying that E4 = E1, I got an answer of zero.
How did you get the answer of zero? What steps of reasoning did you use?
 

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