The fringe width \( \beta \) in a double slit experiment is determined by the formula: \[ \beta = \frac{\lambda D}{d} \] where \( \lambda \) represents the wavelength of the light, \( D \) is the separation between the slits and the screen, and \( d \) is the separation between the slits.
Given \( \lambda = 600 \, \text{nm} = 600 \times 10^{-9} \, \text{m} \), \( D = 1.0 \, \text{m} \), and \( d = 1.0 \, \text{mm} = 1.0 \times 10^{-3} \, \text{m} \), the fringe width is calculated as: \[ \beta = \frac{600 \times 10^{-9} \times 1.0}{1.0 \times 10^{-3}} = 6.0 \times 10^{-4} \, \text{m} \] The distance of the third bright fringe from the central maximum is found by: \[ y_3 = 3 \times \beta = 3 \times 6.0 \times 10^{-4} = 1.8 \times 10^{-3} \, \text{m} = 1.8 \, \text{mm} \] Consequently, the third bright fringe is located 1.8 mm from the center.
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 : 