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Question: There are three identical point sources $S_1$, $S_2$ and $S_3$ of wavelength $\lambda$ each, are pla...

There are three identical point sources S1S_1, S2S_2 and S3S_3 of wavelength λ\lambda each, are placed near a large screen at x=dx=d. If n1n_1, n2n_2 and n3n_3 are number of maxima observed for a pair of sources with third switched off. That means n1n_1 is the number of maxima when s1s_1 switched off; and n2n_2 is the number of maxima when s2s_2 switched off similarly n3n_3 is the number of maxima when S3S_3 switched off. Then (n1+n2+n3)(n_1 + n_2 + n_3), for d=3λd = 3\lambda and a=λa = \lambda, is

A

7

B

5

C

6

D

8

Answer

7

Explanation

Solution

The problem involves calculating the number of maxima observed from pairs of point sources due to interference. The number of maxima for a pair of sources is determined by the range of possible path differences and the condition for constructive interference (Δr=mλ\Delta r = m\lambda).

1. Pair of sources S1S_1 and S2S_2 (n1n_1) Sources are S1=(0,a)S_1=(0, a) and S2=(0,0)S_2=(0, 0). The screen is at x=dx=d. The path difference Δr12\Delta r_{12} can be approximated for a large screen (dad \gg a) as Δr12a22ay2d\Delta r_{12} \approx \frac{a^2 - 2ay}{2d}. For maxima, Δr12=mλ\Delta r_{12} = m\lambda. So, a22ay2d=mλ\frac{a^2 - 2ay}{2d} = m\lambda. The range of path difference is determined by the limits as y±y \to \pm \infty. As y±y \to \pm \infty, Δr12\Delta r_{12} ranges from a-a to aa. So, amλa-a \le m\lambda \le a, which implies aλmaλ-\frac{a}{\lambda} \le m \le \frac{a}{\lambda}. Given a=λa = \lambda, we have 1m1-1 \le m \le 1. The possible integer values for mm are 1,0,1-1, 0, 1. Therefore, n1=3n_1 = 3.

2. Pair of sources S1S_1 and S3S_3 (n2n_2) Sources are S1=(0,a)S_1=(0, a) and S3=(a,0)S_3=(a, 0). The screen is at x=dx=d. The distance between S1S_1 and S3S_3 is s=(a0)2+(0a)2=a2s = \sqrt{(a-0)^2 + (0-a)^2} = a\sqrt{2}. The maximum possible path difference between these two sources is equal to the distance between them, which is a2a\sqrt{2}. So, the range of path difference is from a2-a\sqrt{2} to a2a\sqrt{2}. For maxima, Δr13=mλ\Delta r_{13} = m\lambda. Thus, a2mλa2-a\sqrt{2} \le m\lambda \le a\sqrt{2}, which implies a2λma2λ-\frac{a\sqrt{2}}{\lambda} \le m \le \frac{a\sqrt{2}}{\lambda}. Given a=λa = \lambda, we have 2m2-\sqrt{2} \le m \le \sqrt{2}. The possible integer values for mm are 1,0,1-1, 0, 1. Therefore, n2=3n_2 = 3.

3. Pair of sources S2S_2 and S3S_3 (n3n_3) Sources are S2=(0,0)S_2=(0, 0) and S3=(a,0)S_3=(a, 0). The screen is at x=dx=d. The path difference Δr23\Delta r_{23} can be approximated for a large screen as Δr23aay22d(da)\Delta r_{23} \approx a - \frac{ay^2}{2d(d-a)}. The maximum path difference occurs at y=0y=0, where Δr23(0)=d(da)=a\Delta r_{23}(0) = d - (d-a) = a. As y|y| \to \infty, Δr230\Delta r_{23} \to 0. So, the range of path difference is (0,a](0, a]. For maxima, Δr23=mλ\Delta r_{23} = m\lambda. Thus, 0<mλa0 < m\lambda \le a, which implies 0<maλ0 < m \le \frac{a}{\lambda}. Given a=λa = \lambda, we have 0<m10 < m \le 1. The only possible integer value for mm is 11. Therefore, n3=1n_3 = 1.

The total number of maxima is (n1+n2+n3)=3+3+1=7(n_1 + n_2 + n_3) = 3 + 3 + 1 = 7.