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 capacitors \( C_1 \) and \( C_2 \) are connected in parallel to a battery. Charge-time graph is shown below for the two capacitors. The energy stored with them are \( U_1 \) and \( U_2 \), respectively. Which of the given statements is true? 
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:


