A capacitor of capacitance ‘C’ is charged to a potential ‘V’ and disconnected from the battery. Now if the space between the plates is completely filled with a substance of dielectric constant ‘K’, the final charge and the final potential on the capacitor are respectively:
\( KCV \) and \( \frac{V}{K} \)
\( CV \) and \( \frac{V}{K} \)
\( \frac{CV}{K} \) and \( KV \)
\( \frac{CV}{K} \) and \( \frac{V}{K} \)
Step 1: Understanding the Effect of Dielectric on a Disconnected Capacitor Since the capacitor is disconnected from the battery, its charge remains constant. The charge on the capacitor is given by: \[ Q = C V \] Step 2: Effect of Introducing the Dielectric When a dielectric material with dielectric constant \( K \) is introduced, the capacitance of the capacitor increases as: \[ C' = K C \] However, since the charge remains constant, the new potential \( V' \) across the capacitor is given by: \[ V' = \frac{Q}{C'} = \frac{CV}{KC} = \frac{V}{K} \] Thus, the final charge remains \( CV \), and the new potential is \( \frac{V}{K} \).
Two charges \( +q \) and \( -q \) are placed at points \( A \) and \( B \) respectively which are at a distance \( 2L \) apart. \( C \) is the midpoint of \( AB \). The work done in moving a charge \( +Q \) along the semicircle CSD (\( W_1 \)) and along the line CBD (\( W_2 \)) are 
Find work done in bringing charge q = 3nC from infinity to point A as shown in the figure : 