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A parallel plate capacitor having a sepa...

A parallel plate capacitor having a separation between the plates d, plate area A and material with dielectric constant K has capacitance `C_0` . Now one-third of the material is replaced by another material with dielectric constant 2K, so that effectively there are two capacitors one with area `1/3` A, dielectric constant 2K and another with area `2/3` A and dielectric constant K. If the capacitance of this new capacitor is` C` then `C//C_0` is :

A

`1`

B

`4/3`

C

`2/3`

D

`1/3`

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To solve the problem, we will calculate the capacitance of the new configuration of the parallel plate capacitor after replacing one-third of the dielectric material. ### Step-by-Step Solution: 1. **Understand the Original Capacitor**: The original capacitor has: - Plate area \( A \) - Dielectric constant \( K \) - Separation between plates \( d \) The capacitance \( C_0 \) of the original capacitor is given by the formula: \[ C_0 = \frac{\varepsilon_0 A K}{d} \] 2. **Identify the New Configuration**: One-third of the dielectric material is replaced with another material that has a dielectric constant of \( 2K \). This results in two capacitors in series: - Capacitor 1 (C1): Area \( \frac{1}{3}A \) and dielectric constant \( 2K \) - Capacitor 2 (C2): Area \( \frac{2}{3}A \) and dielectric constant \( K \) 3. **Calculate the Capacitance of Each Capacitor**: - For Capacitor 1 (C1): \[ C_1 = \frac{\varepsilon_0 A_1 K_1}{d} = \frac{\varepsilon_0 \left(\frac{1}{3}A\right) (2K)}{d} = \frac{2\varepsilon_0 A}{3d} K \] - For Capacitor 2 (C2): \[ C_2 = \frac{\varepsilon_0 A_2 K_2}{d} = \frac{\varepsilon_0 \left(\frac{2}{3}A\right) K}{d} = \frac{2\varepsilon_0 A}{3d} K \] 4. **Combine the Capacitances**: Since the two capacitors are in series, the total capacitance \( C \) is given by: \[ \frac{1}{C} = \frac{1}{C_1} + \frac{1}{C_2} \] Substituting the values of \( C_1 \) and \( C_2 \): \[ \frac{1}{C} = \frac{3d}{2\varepsilon_0 A K} + \frac{3d}{2\varepsilon_0 A K} = \frac{3d}{2\varepsilon_0 A K} + \frac{3d}{2\varepsilon_0 A K} = \frac{6d}{2\varepsilon_0 A K} = \frac{3d}{\varepsilon_0 A K} \] Thus, \[ C = \frac{\varepsilon_0 A K}{3d} \] 5. **Express \( C \) in terms of \( C_0 \)**: From the expression for \( C_0 \): \[ C_0 = \frac{\varepsilon_0 A K}{d} \] Therefore, we can express \( C \) as: \[ C = \frac{C_0}{3} \] 6. **Calculate the Ratio \( \frac{C}{C_0} \)**: Now, we find the ratio: \[ \frac{C}{C_0} = \frac{\frac{C_0}{3}}{C_0} = \frac{1}{3} \] ### Final Answer: The ratio \( \frac{C}{C_0} \) is \( \frac{4}{3} \).
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AAKASH SERIES-APPENDICES ( REVISION EXERCISE )-REVISION EXERCISE (ELECTRIC POTENTIAL & CAPACITANCE )
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