Coherent sources: Coherent sources are those sources which emit continuously light of the same wavelength and magnitude either in the same phase or with a constant phase difference.
Expression
Let the waves of two coherent sources be
y1 = a sin ωt
and y2 = b sin (ωt + Φ),
where a and b are the respective amplitudes of the two waves and Φ is the constant phase angle by which the second wave leads the first wave [Fig].
According to superposition principle, the displacement y of resultant wave is
y = y1 + y2 = a sin ωt + b sin (ωt + Φ)
or y = a sin ωt + b sin ωt cos Φ + b cos ωt sin Φ
or y = sin ωt (a + b cos Φ) + cos ωt. b sin Φ
Substituting a + b cos Φ = A cos θ ..........(1)
and b sin Φ = A sin θ ..........(2)
we have
y = sin ωt. A cos θ + cos ωt. A sin θ
or y = A [sin ωt. cos θ + cos ωt. sin θ]
or y = A sin (ωt + θ),
where A is the amplitude of the resultant wave. Squaring and adding (1) and (2), we have
a2 + b2 cos2 Φ + 2ab cos Φ + b2 sin2 Φ
= A2 cos2 θ + A2 sin2 θ
or a2 + b2 (cos2 Φ + sin2 Φ + 2ab cos θ)
= A2 (cos2 θ + sin2 θ)
or A2 = a2 + b2 + 2ab cos Φ

Since resultant intensity is proportional to square of amplitude,
∴ I ∝ A2
or I ∝ (a2 + b2 + 2ab cos Φ)
or I = a2 + b2 + 2 ab cos Φ ............(3)
(For convenience, we assume that intensity of light is equal to square of amplitude)
(i) For constructive interference (or for maximum).
I should be maximum
i.e. cos Φ = 1 and Imax = (a + b)2
or Φ = 0, 2π, 4π, ...........
or Φ = 2π n (where n = 0, 1, 2, ..........)
or Path diff. = \(\frac{\lambda}{2\pi} \phi = \frac{\lambda}{2\pi} \) 2πn = n λ ..........(4)
So, for constructive interference (or for maximum intensity), path difference should be integral multiple of λ.
(ii) For destructive interference (or for minima)
I should be minimum
i.e. cos Φ = -1 and Imin = (a - b)2
or Φ = π, 3π, 5π, ..........................
or Φ = (2n + 1) π (where n = 0, 1, 2, ..........)
or path difference = \(\frac{\lambda}{2\pi} (2n + 1) \pi\)
= (2n + 1) \(\frac{\lambda}{2}\) ...............(5)
So, for destructive interference (or for minimum intensity), path difference should be an odd multiple of λ/2.
Variation of intensity with position
From above discussion, we find that intensity of light is maximum when path difference is nλ i.e. ±λ, 2λ, 3λ .......... and minimum when path difference is (2 n+ 1) λ/2
i.e. ± \(\frac{\lambda}{2}, 3\frac{\lambda}{2}, 5\frac{\lambda}{2}\)
The variation in intensity of light with position in interference is as shown in Fig. (b).
