Question
Question: A source \( S \) and a detector \( D \) of high frequency waves are a distance \( d \) apart on the ...
A source S and a detector D of high frequency waves are a distance d apart on the ground. The direct wave from S is found to be in phase at D with the wave from S that is reflected rays making the same angle with the reflecting layer. When the layer rises a distance h , no signal is detected at D . Neglect absorption in the atmosphere and find the relation between d , h , H and the wavelength λ of the waves.
Solution
Hint : In order to solve this question, we are going to consider the two rays that are approaching the point D first from the height H and then from the height (H+h) . 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
The path difference for destructive interference is given by
Δx=(n+21)λ .
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 H , and the other one comes to D 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
Where,
n=0,1,2,3,....
Let us consider a point P at the height H
Thus, SD=d
SP=H2+(2d)2
And, PD=H2+(2d)2
Hence, SP+PD=2H2+(2d)2=4H2+d2
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+h , there is no direct ray coming to D , then the destructive interference occurs at D
Now, path difference for destructive interference is given by
Δx=(n+21)λ
Where, n=0,1,2,3,....
Let us consider a point Q at the height H+h
SD=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+(2d)2=4(H+h)2+d2
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) from equation (2)
λ=24(H+h)2+d2−24H2+d2
Note :
For both the constructive and the destructive interference, two factors that remain common are the variable n 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.