Two identical radiators have a separation of where is the wavelength of the waves emitted by either source. The initial phase difference between the sources is . Then the intensity on the screen at a distant point situated at an angle from the radiators is (here I0 is intensity at that point due to one radiator alone)
The intensity at a point on screen is given by
where is the phase difference. In this problem arises (i) due to initial phase difference of and (ii) due to path difference for the observation point situated at Thus
Thus