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Question: A parallel plate capacitor of capacitance $C$ (without dielectrics) is filled by dielectric slabs as...

A parallel plate capacitor of capacitance CC (without dielectrics) is filled by dielectric slabs as shown in the figure. Then the new capacitance of the capacitor is:

A

3.9 CC

B

4 CC

C

2.4 CC

D

3 CC

Answer

4 CC

Explanation

Solution

The capacitor can be considered as two capacitors in series. The top capacitor has a dielectric constant of 6 and thickness d. The bottom capacitor is made of two capacitors in parallel, with dielectric constants 2 and 4, each with thickness d.

The capacitance of the top capacitor is Ctop=6ϵ0AdC_{top} = \frac{6\epsilon_0 A}{d}. The capacitance of the left part of the bottom capacitor is C1=2ϵ0(A/2)d=ϵ0AdC_1 = \frac{2\epsilon_0 (A/2)}{d} = \frac{\epsilon_0 A}{d}. The capacitance of the right part of the bottom capacitor is C2=4ϵ0(A/2)d=2ϵ0AdC_2 = \frac{4\epsilon_0 (A/2)}{d} = \frac{2\epsilon_0 A}{d}. The capacitance of the bottom capacitor is Cbottom=C1+C2=ϵ0Ad+2ϵ0Ad=3ϵ0AdC_{bottom} = C_1 + C_2 = \frac{\epsilon_0 A}{d} + \frac{2\epsilon_0 A}{d} = \frac{3\epsilon_0 A}{d}.

The equivalent capacitance is given by 1Ceq=1Ctop+1Cbottom=d6ϵ0A+d3ϵ0A=d6ϵ0A+2d6ϵ0A=3d6ϵ0A=d2ϵ0A\frac{1}{C_{eq}} = \frac{1}{C_{top}} + \frac{1}{C_{bottom}} = \frac{d}{6\epsilon_0 A} + \frac{d}{3\epsilon_0 A} = \frac{d}{6\epsilon_0 A} + \frac{2d}{6\epsilon_0 A} = \frac{3d}{6\epsilon_0 A} = \frac{d}{2\epsilon_0 A}. Therefore, Ceq=2ϵ0AdC_{eq} = \frac{2\epsilon_0 A}{d}.

The original capacitance is C=ϵ0A2dC = \frac{\epsilon_0 A}{2d}. Thus, Ceq=2ϵ0Ad=4ϵ0A2d=4CC_{eq} = \frac{2\epsilon_0 A}{d} = 4\frac{\epsilon_0 A}{2d} = 4C.