Conditions of constructive interference and destructive interference.
consider two coherent waves travelling in the same direction along a straight line.
Frequency of each wave is given by \(\frac{\omega}{2\pi},\)
Amplitude of electric field vectors are a1 and a2 respectively.
Wave equation is represented by,
y1 = a1 sin ωt ....(i)
y2 = a2 sin (ωt + ϕ) ....(ii)
Using the theory of superposition,
y = y1 + y2 .....(iii)
Here, y1 and y2 are the points of electric field.
Putting values from (ii) and (iii) in (i), we have
y = a1 sin ωt + a2 sin (ωt + ϕ)
Now using trignometric identities, we have
sin (ωt + ϕ) = sin ωt cos ϕ + cos ωt sin ϕ
we get,
y = a1 sin ωt + a2 (sin ωt cos ϕ + cos ωt sin ϕ)
= (a1 + a2 cos ϕ) sin ωt + (a2 sin ϕ) cos ωt ....(iv)
Assume,
a1 + a2 cos ϕ = A cos θ
and
a2 sin ϕ = A sin θ
so, eqn. (iv) gives,
y = A cos θ sin ωt + A sin θ cos ωt
= A sin (ωt + ϕ)
Amplitude of the resultant wave is given by,
Amplitude, \(A = \sqrt{a_1{^2} + a_2{^2} + 2a_1a_2 \cos \phi}\)
Intensity of the wave is proportional to the amplitude of the wave.
Thus, intensity of the resultant wave is given by,
I = A2 = a12 + a22 + 2a1a2 cos ϕ
Constructive interference : For maximum intensity at any point, cos = +1
phase difference, ϕ = 0, 2π, 4π, 6π, .......
= 2nπ(n = 0, 1, 2, ....)
So, maximum intensity is,
Imax = a12 + a22 + 2a1a2 = (a1 + a2)2
Path difference is,
Δ \(= \frac{\lambda}{2\pi}\) × Phase difference \(= \frac{\lambda}{2\pi}\) × 2nπ = nλ
Constructive interference is obtained when the path difference between the waves is an integral multiple of λ
Destructive interference : For minimum intensity at any point, cos = -1
phase difference is given by,
ϕ = π, 3π, 5π, 7π, .......
= (2n -1) π, n = 1, 2, 3, .....
Minimum intensity is,
Imin = a12 + a22 - 2a1a2 = (a1 - a2)2
Path difference is,
Δ \(= \frac{\lambda}{2\pi}\) × Phase difference
\(= \frac{\lambda}{2\pi}\) × (2n - 1) π = (2n - 1)\(\frac{\lambda}{2}\)
In destructive interference, path difference is odd multiple of \(\frac{\lambda}{2}.\)