A parallel plate capacitor is filled equally (half) with two dielectrics of dielectric constant $ \epsilon_1 $ and $ \epsilon_2 $, as shown in figures. The distance between the plates is d and area of each plate is A. If capacitance in first configuration and second configuration are $ C_1 $ and $ C_2 $ respectively, then $ \frac{C_1}{C_2} $ is:
Let \( C_0 = \frac{\epsilon_0 A}{d} \)
First Configuration: Area of plate is A.
Then \( C = \frac{\epsilon_2 \epsilon_0 A}{d/2} = \frac{2\epsilon_2 \epsilon_0 A}{d} = 2\epsilon_2 C_0 \) \( C' = \frac{\epsilon_1 \epsilon_0 A}{d/2} = \frac{2\epsilon_1 \epsilon_0 A}{d} = 2\epsilon_1 C_0 \) C and C' are in series.
\( C_1 = \frac{CC'}{C+C'} = \frac{4\epsilon_1 \epsilon_2 C_0^2}{2C_0 (\epsilon_2 + \epsilon_1)} \)
\( C_1 = \frac{2\epsilon_2 \epsilon_1 C_0}{(\epsilon_2 + \epsilon_1)} \)
Second Configuration:
Here \( C = \frac{\epsilon_1 \epsilon_0 A}{2d} = \frac{\epsilon_1 C_0}{2} \)
\( C' = \frac{\epsilon_2 C_0}{2} \) C and C' are in parallel.
\( C_2 = C' + C = (\epsilon_1 + \epsilon_2) \frac{C_0}{2} \)
Thus \( \frac{C_1}{C_2} = \frac{2\epsilon_1 \epsilon_2 C_0}{(\epsilon_2 + \epsilon_1)} \times \frac{2}{(\epsilon_1 + \epsilon_2) C_0} \) \( \frac{C_1}{C_2} = \frac{4\epsilon_1 \epsilon_2}{(\epsilon_2 + \epsilon_1)^2} \)
Two charges $ q_1 $ and $ q_2 $ are separated by a distance of 30 cm. A third charge $ q_3 $ initially at C as shown in the figure, is moved along the circular path of radius 40 cm from C to D. If the difference in potential energy due to the movement of $ q_3 $ from C to D is given by $ \frac{q_3 K}{4 \pi \epsilon_0} $, the value of $ K $ is:
Three parallel plate capacitors $ C_1 $, $ C_2 $, and $ C_3 $ each of capacitance 5 µF are connected as shown in the figure. The effective capacitance between points A and B, when the space between the parallel plates of $ C_1 $ capacitor is filled with a dielectric medium having dielectric constant of 4, is:
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