Two identical sources, each of intensity I0, have a separation d=λ/8, where λ is the wavelength of the waves emitted by either source. The phase difference of the sources is π/4. The intensity distribution I(θ) in the radiation field, as a function of θ, which specifies the direction from the sources to the distant observation point P, is given by
(1) I(θ)=I0cos2θ
(2) I(θ)=4I0cos2(8πθ)
(3) I(θ)=4I0cos2[8π(sinθ+1)]
(4) I(θ)=I0sin2θ