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Question: A source \( S \) and a detector \( D \) of high frequency waves are a distance \( d \) apart on the ...

A source SS and a detector DD of high frequency waves are a distance dd apart on the ground. The direct wave from SS is found to be in phase at DD with the wave from SS that is reflected rays making the same angle with the reflecting layer. When the layer rises a distance hh , no signal is detected at DD . Neglect absorption in the atmosphere and find the relation between dd , hh , HH and the wavelength λ\lambda of the waves.

Explanation

Solution

Hint : In order to solve this question, we are going to consider the two rays that are approaching the point DD first from the height HH and then from the height (H+h)\left( {H + h} \right) . The first one will form constructive interference and the latter will be destructive. Thus, respective path differences are subtracted.
The path difference for constructive interference is given by
Δx=nλ\Delta x = n\lambda
The path difference for destructive interference is given by
Δx=(n+12)λ\Delta x = \left( {n + \dfrac{1}{2}} \right)\lambda .

Complete Step By Step Answer:
If we observe the situation as given in the question, we see that when a ray is reflected from a height HH , and the other one comes to DD in a direct way, then, the interference that occurs is a constructive one.
We know that the path difference for constructive interference is given by
Δx=nλ\Delta x = n\lambda
Where,
n=0,1,2,3,....n = 0,1,2,3,....
Let us consider a point P at the height HH
Thus, SD=dSD = d
SP=H2+(d2)2SP = \sqrt {{H^2} + {{\left( {\dfrac{d}{2}} \right)}^2}}
And, PD=H2+(d2)2PD = \sqrt {{H^2} + {{\left( {\dfrac{d}{2}} \right)}^2}}
Hence, SP+PD=2H2+(d2)2=4H2+d2SP + PD = 2\sqrt {{H^2} + {{\left( {\dfrac{d}{2}} \right)}^2}} = \sqrt {4{H^2} + {d^2}}
Hence, the path difference is given by
\Delta x = SP - SD = \sqrt {4{H^2} + {d^2}} - d \\\ \Rightarrow n\lambda = \sqrt {4{H^2} + {d^2}} - d - - - - \left( 1 \right) \\\
When ray comes from height H+hH + h , there is no direct ray coming to DD , then the destructive interference occurs at DD
Now, path difference for destructive interference is given by
Δx=(n+12)λ\Delta x = \left( {n + \dfrac{1}{2}} \right)\lambda
Where, n=0,1,2,3,....n = 0,1,2,3,....
Let us consider a point Q at the height H+hH + h
SD=dSD = d
And
SQ = \sqrt {{{\left( {H + h} \right)}^2} + {{\left( {\dfrac{d}{2}} \right)}^2}} \\\ QD = \sqrt {{{\left( {H + h} \right)}^2} + {{\left( {\dfrac{d}{2}} \right)}^2}} \\\
Thus, SQ+QD=2(H+h)2+(d2)2=4(H+h)2+d2SQ + QD = 2\sqrt {{{\left( {H + h} \right)}^2} + {{\left( {\dfrac{d}{2}} \right)}^2}} = \sqrt {4{{\left( {H + h} \right)}^2} + {d^2}}
Hence, the path difference is given by
SQ - SD = \sqrt {4{{\left( {H + h} \right)}^2} + {d^2}} - d \\\ \Rightarrow \left( {n + \dfrac{1}{2}} \right)\lambda = \sqrt {4{{\left( {H + h} \right)}^2} + {d^2}} - d - - - - \left( 2 \right) \\\
Subtracting equation (1)\left( 1 \right) from equation (2)\left( 2 \right)
λ=24(H+h)2+d224H2+d2\lambda = 2\sqrt {4{{\left( {H + h} \right)}^2} + {d^2}} - 2\sqrt {4{H^2} + {d^2}}

Note :
For both the constructive and the destructive interference, two factors that remain common are the variable nn and the wavelength, the respective relations for both the types are different which gives two different equations and thus, helps to solve for the value of the wavelength.