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A parallel plate capacitor (condenser) h...

A parallel plate capacitor (condenser) has a certain capacitance (capacity). When 2/3 rd of the distance between the plates is filled with a dielectric, the (capacity) capacitance is found to be 2.25 times the initial capacitance. The dielectric constant of the dielectric

A

1

B

3

C

7

D

6

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The correct Answer is:
To solve the problem of finding the dielectric constant \( k \) of a dielectric material that fills \( \frac{2}{3} \) of the distance between the plates of a parallel plate capacitor, we can follow these steps: ### Step 1: Understand the initial capacitance The initial capacitance \( C \) of a parallel plate capacitor with air (or vacuum) between the plates is given by: \[ C = \frac{A \epsilon_0}{d} \] where \( A \) is the area of the plates, \( \epsilon_0 \) is the permittivity of free space, and \( d \) is the distance between the plates. ### Step 2: Define the new configuration When \( \frac{2}{3} \) of the distance \( d \) is filled with a dielectric of dielectric constant \( k \), the capacitor can be thought of as two capacitors in series: 1. Capacitor \( C_1 \) (with dielectric) has a distance of \( \frac{2}{3}d \). 2. Capacitor \( C_2 \) (without dielectric) has a distance of \( \frac{1}{3}d \). ### Step 3: Calculate the capacitances of the two sections The capacitance of \( C_1 \) is: \[ C_1 = \frac{A k \epsilon_0}{\frac{2}{3}d} = \frac{3A k \epsilon_0}{2d} \] The capacitance of \( C_2 \) is: \[ C_2 = \frac{A \epsilon_0}{\frac{1}{3}d} = 3A \epsilon_0 \] ### Step 4: Use the formula for capacitors in series The total capacitance \( C' \) of the two capacitors in series is given by: \[ \frac{1}{C'} = \frac{1}{C_1} + \frac{1}{C_2} \] Substituting the values of \( C_1 \) and \( C_2 \): \[ \frac{1}{C'} = \frac{2d}{3A k \epsilon_0} + \frac{1}{3A \epsilon_0} \] ### Step 5: Find a common denominator The common denominator is \( 3A k \epsilon_0 \): \[ \frac{1}{C'} = \frac{2d + k d}{3A k \epsilon_0} = \frac{(2 + k)d}{3A k \epsilon_0} \] Thus, \[ C' = \frac{3A k \epsilon_0}{(2 + k)d} \] ### Step 6: Relate the new capacitance to the initial capacitance According to the problem, the new capacitance \( C' \) is 2.25 times the initial capacitance \( C \): \[ C' = 2.25 C \] Substituting the expression for \( C' \): \[ \frac{3A k \epsilon_0}{(2 + k)d} = 2.25 \cdot \frac{A \epsilon_0}{d} \] ### Step 7: Simplify the equation Cancel \( A \epsilon_0/d \) from both sides: \[ \frac{3k}{2 + k} = 2.25 \] ### Step 8: Solve for \( k \) Cross-multiplying gives: \[ 3k = 2.25(2 + k) \] Expanding the right side: \[ 3k = 4.5 + 2.25k \] Rearranging: \[ 3k - 2.25k = 4.5 \implies 0.75k = 4.5 \] Thus, \[ k = \frac{4.5}{0.75} = 6 \] ### Final Answer The dielectric constant \( k \) is \( 6 \). ---
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AAKASH SERIES-APPENDICES ( REVISION EXERCISE )-REVISION EXERCISE (ELECTRIC POTENTIAL & CAPACITANCE )
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