Step 1: The capacitance of a parallel plate capacitor is given by the formula: \[ C = \frac{\varepsilon_0 A}{d} \] where \( \varepsilon_0 \) is the permittivity of free space, \( A \) is the area of the plates, and \( d \) is the separation between the plates.
Step 2: When the distance \( d \) between the plates is halved, the capacitance doubles. Moreover, when a dielectric material is inserted, the capacitance increases by the factor of the dielectric constant \( K \).
Step 3: The new capacitance is: \[ C' = K \times \frac{C}{2} \] where \( K = 3 \) and \( C = 1.5 \, \mu F \). \[ C' = 3 \times \frac{1.5}{2} = 9 \, \mu F \]
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 : 