Let \( A \) denote the prism angle, \( i \) the angle of incidence on face AB, and \( e \) the angle of emergence. The deviation angle \( D \) is the angle between the incident and emergent rays. We are given \( D = 15^\circ \) and \( A = 30^\circ \). The formula for deviation in a prism is \( D = i + e - A \). Since the emergent ray is normal to face AC, \( e = 90^\circ \). Substituting these values: \( 15^\circ = i + 90^\circ - 30^\circ \). Solving for \( i \) yields \( i = 15^\circ \). Snell's law, \( n = \frac{\sin(i)}{\sin(r)} \), is used to determine the refractive index \( n \) of the prism material, where \( r \) is the angle of refraction within the prism. Given \( r = 90^\circ - A/2 \), substituting known values allows calculation of the refractive index.
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 : 