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Question: Two large metal sheets having surface charge density $+\sigma/2$ and $-\sigma/2$ are kept parallel t...

Two large metal sheets having surface charge density +σ/2+\sigma/2 and σ/2-\sigma/2 are kept parallel to each other at a small separation distance d. The electric field at any point in the region between the plates is

A

σ/2ϵ0\sigma/2\epsilon_0

B

σ/ϵ0\sigma/\epsilon_0

C

σ/4ϵ0\sigma/4\epsilon_0

D

2σ/ϵ02\sigma/\epsilon_0

Answer

σ/2ϵ0\sigma/2\epsilon_0

Explanation

Solution

The electric field due to a single infinite sheet with surface charge density ρs\rho_s is E=ρs2ϵ0E = \frac{|\rho_s|}{2\epsilon_0}.

For the positive sheet (+σ/2+\sigma/2), the field is E1=σ/22ϵ0=σ4ϵ0E_1 = \frac{\sigma/2}{2\epsilon_0} = \frac{\sigma}{4\epsilon_0}, directed away from it.

For the negative sheet (σ/2-\sigma/2), the field is E2=σ/22ϵ0=σ4ϵ0E_2 = \frac{|-\sigma/2|}{2\epsilon_0} = \frac{\sigma}{4\epsilon_0}, directed towards it.

Between the plates, both fields point in the same direction.

Total electric field Etotal=E1+E2=σ4ϵ0+σ4ϵ0=σ2ϵ0E_{total} = E_1 + E_2 = \frac{\sigma}{4\epsilon_0} + \frac{\sigma}{4\epsilon_0} = \frac{\sigma}{2\epsilon_0}.