Two planes of charge with no thickness, A and B, are parallel and vertical. The electric field in region I to the left of plane A has magnitude 3σ/2????0 and points to the left. The electric field in the region to the right of B has magnitude 3σ/2????0 and points to the right. The electric field in the region between the two planes has magnitude σ/2????0 and points to the right. The surface charge density on planes A and B respectively is

Answer :

Answer:

The surface charge density on planes A and B respectively is

     [tex]\sigma__{A}} } = 2\sigma[/tex]

and

     [tex]\sigma__{B}} = \sigma[/tex]

Explanation:

From the question we are told that

     The  electric field in region to the left of  A  is  [tex]E_i = \frac{3 \sigma}{2 \epsilon_o}[/tex]

      The  direction of the electric field is  left

      The  electric field in the region to the right of  B  is  [tex]E_f = \frac{3 \sigma}{2 \epsilon_o}[/tex]

      The  direction of the electric field is  right

      The  electric field in the region between the two planes is  [tex]E_m = \frac{\sigma }{2 \epsilon_o }[/tex]

       The  direction of the electric field is  right

Let the surface charge density on planes A and B be represented as [tex]\sigma__{A}} \ \ and \ \ \sigma__{B}} \ \ \ respectively[/tex]

 From the question we see that

         [tex]E_i = E_f[/tex]

Generally the electric to the right and to the left is due to the combined electric field generated by  plane  A and  B  so

         [tex]E_i = E_f = \frac{3\sigma }{2\epsilon} = \frac{\sigma_A }{ 2 \epsilon_o } + \frac{\sigma_B }{ 2 \epsilon_o }[/tex]

=>      [tex]\sigma__{A}} + \sigma__{B}} = 3 \sigma -- -(1)[/tex]

Generally the electric field at the middle of the plane A and  B  is due to the diffencence in electric field generated by plane A and  B      

i.e

          [tex]\frac{\sigma }{2 \epsilon_o } = \frac{\sigma_A }{ 2 \epsilon_o } - \frac{\sigma_B }{ 2 \epsilon_o }[/tex]

=>      [tex]\sigma__{A}} - \sigma__{B}} = \sigma[/tex]

=>      [tex]\sigma__{A}} } = \sigma + \sigma__{B}[/tex]

From equation 1

        [tex]\sigma + \sigma__{B}}+ \sigma__{B}} = 3 \sigma[/tex]

=>    [tex]\sigma__{B}} = \sigma[/tex]

So

      [tex]\sigma__{A}} } = \sigma + \sigma[/tex]

=>   [tex]\sigma__{A}} } = 2\sigma[/tex]

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