When waves from two coherent sources, having amplitudes a and b superimpose, the amplitude R of the resultant wave is given by :
= \(\sqrt{a^2+b^2+2ab\,cosϕ}\),
Where φ is the constant phase angle between the two waves.
The resultant intensity I is directly proportional to the square of the amplitude of the resultant wave,
I.e. I∝(R2)
I.e. I ∝ (a2 + b2 + 2ab cosϕ)
For constructive interference,
φ = 2nπ,
Imax = (a + b)2
For destructive interference,
φ = (2n-1)π
Imin = (a − b)2
If, I1 and I2 are intensities of light from two slits of widths, w1 and w2,
Then,
\(\frac{I_1}{I_2}\) = \(\frac{w_1}{w_2}\) = \(\frac{a^2}{b^2}\)
Light waves from two coherent sources of intensity ratio 81:1 produce interference.
(i) The ratio of amplitudes of two sources is :
(a) 9:1
(b) 81:1
(c) 1:9
(d) 1:81
(ii) The ratio of slit widths of the two sources is :
(a) 9:1
(b) 81:1
(c) 1:9
(d) 1:81
(iii) The ratio of maxima and minima in the interference pattern is :
(a) 9:1
(b) 81:1
(c) 25:16
(d) 16:25
(iv) If two slits in Young’s experiment have width ratio 1:4, the ratio of maximum and minimum intensity in the interference pattern would be :
(a) 1:4
(b)1:16
(c) 9:1
(d) 9:16