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Question
Two coherent narrow slits emitting sound of wavelength λ in the same phase are placed parallel to each other at a small separation of 2λ. The sound is detected by moving a detector on the screen ∑ at a distance D(>>λ) from the slit S1 as shown in figure. Find the distance x such that the intensity at P is equal to the intensity at O.
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Solution
Given:
S1& S2 are in the same phase. At O, there will be maximum intensity.
There will be maximum intensity at P.

\[∆ S_1 PO\] and \[∆ S_2 PO\] are right-angled triangles.
So,
\[\left( S_1 P \right)^2 - \left( S_2 P \right)^2 \]
\[ = \left[ D^2 + x^2 \right] - \left[ \left( D - 2\lambda \right)^2 + x^2 \right]^2 \]
\[ = 4\lambda D + 4 \lambda^2 = 4\lambda D\]
\[( \lambda^2 \text { is small and can be neglected })\]
\[ \Rightarrow \left( S_1 P + S_2 P \right)\left( S_1 P - S_2 P \right) = 4\lambda D\]
\[ \Rightarrow \left( S_1 P - S_2 P \right) = \frac{4\lambda D}{\left( S_1 P + S_2 P \right)}\]
\[ \Rightarrow S_1 P - S_2 P = \frac{4\lambda D}{2\sqrt{x^2 + D^2}}\]
For constructive interference, path difference = n \[\lambda\]
So,
\[\Rightarrow S_1 P - S_2 P = \frac{4\lambda D}{2\sqrt{x^2 + D^2}} = n\lambda\]
\[ \Rightarrow \frac{2D}{\sqrt{x^2 + D^2}} = n\]
\[ \Rightarrow n^2 ( x^2 + D^2 ) = 4 D^2 \]
\[ \Rightarrow n^2 x^2 + n^2 D^2 = 4 D^2 \]
\[ \Rightarrow n^2 x^2 = 4 D^2 - n^2 D^2 \]
\[ \Rightarrow n^2 x^2 = D^2 \left( 4 - n^2 \right)\]
\[ \Rightarrow x = \frac{D}{n}\sqrt{4 - n^2}\]
\[\text { When n = 1 }, \]
\[x = \sqrt{3}D (\text { 1st order }) . \]
\[\text { When n } = 2, \]
\[x = 0 \ (\text { 2nd order }) . \]
So, when x = \[\sqrt{3}D\] , the intensity at P is equal to the intensity at O.
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