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Question: The capacitance between adjacent plates shown in the Fig is \[50nF\]. A \(1\mu C\)charge is placed o...

The capacitance between adjacent plates shown in the Fig is 50nF50nF. A 1μC1\mu Ccharge is placed on the middle plate. Find the charge on the outer surface of the upper plate and the potential difference between upper and middle plates:

(A) 0.5μC,10V0.5\mu C,10V
(B) 1μC,20V1\mu C,20V
(C) 0.5μC,20V0.5\mu C,20V
(D) 1.0μC,40V1.0\mu C,40V

Explanation

Solution

Hint
When a charge 1μC1\mu C is placed on the middle plate, a charge is formed on both the upper and lower surface of all the plates. Since the charge gets equally distributed, we can find the charge on the outer surface of the upper plate from there.
In this, we will use the formula,
Electric Field = Qtotal2Sεo{\text{Electric Field = }}\dfrac{{{Q_{total}}}}{{2S{\varepsilon _o}}}
where Qtotal{Q_{total}} is the sum of all the charges, SS is the surface area of the plates , εo{\varepsilon _o} is permittivity in free space
and, V=QCV = \dfrac{Q}{C}
Where, VV is the potential difference, QQ is the charge on the plate, CC is the capacitance.

Complete Step by Step Solution

According to the problem, there are 3 parallel plates and the capacitance between them is given 50nF50nF. Now, we place a charge 1μC1\mu C inside the middle plate.
On placing the charge 1μC1\mu C at P, it spreads throughout the second plate and all of the plates acquire a positive charge on both its surfaces. The plate AA as a result acquires a negative charge on the lower surface and the plate CC acquires a negative charge on the upper surface. So, the outer surface of AA and the lower surface of CC acquires a positive charge.
The electric field is zero between the plates. Hence,
Qtot2Sεo=0\dfrac{{{Q_{tot}}}}{{2S{\varepsilon _o}}} = 0
12Sεo[qAqA+1qBqB+qCqC]=0\Rightarrow \dfrac{1}{{2S{\varepsilon _o}}}\left[ {{q_A} - {q_A} + 1 - {q_B} - {q_B} + {q_C} - {q_C}} \right] = 0
where qA,qB{q_A},{q_B} and qC{q_C} are the charges on the upper and lower surfaces of plates A,BA,B and CC respectively.
So, from here by doing the calculation, we see that qA{q_A} and qC{q_C} both get cancelled.
2qB=1\therefore 2{q_B} = 1
qB=0.5C\Rightarrow {q_B} = 0.5C
Thus, the charge on the upper surface of BB is
1qB=0.5C1 - {q_B} = 0.5C
The charge on the lower surface of AA is equal and opposite to that of the upper surface of BB.
So,
qA=0.5C- {q_A} = - 0.5C
From the figure, the upper surface of AA has a charge qA=0.5C{q_A} = 0.5C.
To find the potential between the 2 plates, we use the formula, V=qACV = \dfrac{{{q_A}}}{C}.
So putting the values in the above equation, we get
V=0.5×10650×109=10VV = \dfrac{{0.5 \times {{10}^{ - 6}}}}{{50 \times {{10}^{ - 9}}}} = 10V
Thus, the answer to the charge on the outer surface of the upper plate is 0.5μC0.5\mu C and the potential between the upper and middle plate is 10V.
Correct option is (A).

Note
If the external charge had been negative, the charge would be negative on the plate BB and hence, the upper surface of the plate AA would have been different. So, we should be careful about the sign. But the value of the potential would have remained the same.