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

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SUMMARY

The electric field at regions 2 and 3 of the three parallel planes of charge with surface charge densities (-1/2)η, η, and (-1/2)η can be determined using the principle of superposition. The electric field in region 2 points upward, while in region 3, it points downward. The electric field due to a single infinite plane of charge density η is given by the formula E = η/(2ε₀), not η/ε₀. Understanding this distinction is crucial for accurately calculating the electric fields in these regions.

PREREQUISITES
  • Understanding of electric fields generated by infinite planes of charge
  • Familiarity with the principle of superposition in electrostatics
  • Knowledge of surface charge density and its units
  • Basic grasp of ε₀ (epsilon naught) in electrostatics
NEXT STEPS
  • Study the derivation of the electric field due to an infinite plane of charge
  • Learn about the superposition principle in electrostatics
  • Explore the concept of electric field lines and their directionality
  • Review problems involving multiple charged planes and their electric fields
USEFUL FOR

Students studying electrostatics, physics educators, and anyone seeking to understand electric fields generated by charged planes.

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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