Figure here shows P and Q as two equally intense coherent sources emitting radiations of wavelength 20 m. The separation PQ is 5.0 m and phase of P is ahead of the phase of Q by 90∘. A, B and C are three distant points of observation equidistant from the midpoint of PQ. The intensity of radiations at A, B, C will bear the ratio
[NSEP 1994]
2 : 1 : 0
Since P is ahead of Q by 90∘ and path difference between P and Q is λ/4 (As λ = 20m and PQ= 5m); therefore at A, phase difference induced due to path difference PQ is given by, Δϕ=2πλΔx = 2πλ(λ/4) = π/2 = 90∘ (it is negetive as wave from P will be behind wave from Q), hence the total phase difference is zero, so intensity is 4I. At C intensity is zero as total phase difference = 180∘ and at B, the phase difference is 90∘, so intensity is 4Icos2(90∘2)=2I. So, the ratio of intensities at A, B, C is 2:1:0.