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Question: Sound of wavelength \( \lambda \) passes through a Quincke’s tube, which is adjusted to give a minim...

Sound of wavelength λ\lambda passes through a Quincke’s tube, which is adjusted to give a minimum intensity of I0{I_0} .The two interfering waves have equal intensity. Find the minimum distance through the sliding tube should be moved to give an intensity I02\dfrac{{{I_0}}}{2}
(A) λ8\dfrac{\lambda }{8}
(B) λ4\dfrac{\lambda }{4}
(C) 2λ5\dfrac{{2\lambda }}{5}
(D) λ12\dfrac{\lambda }{{12}}

Explanation

Solution

For a Quincke’s tube the maximum intensity of sound occurs only during constructive interference. The intensity of two sound waves in interference is given by I=I1+I2+2I1I2cosϕI = {I_1} + {I_2} + 2\sqrt {{I_1}{I_2}} \cos \phi . Also, the path difference is related to the phase difference by Δx=λ2πΔϕ\Delta x = \dfrac{\lambda }{{2\pi }}\Delta \phi .

Formulas Used: We will be using I=I1+I2+2I1I2cosϕI = {I_1} + {I_2} + 2\sqrt {{I_1}{I_2}} \cos \phi where II is the intensity of interference, I1{I_1} and I2{I_2} are the intensity of the waves that are involved in the interference and ϕ\phi is the phase angle at which the interference occurs. We will also be using Δx=λ2πΔϕ\Delta x = \dfrac{\lambda }{{2\pi }}\Delta \phi where Δx\Delta x is the path difference, λ\lambda is the wavelength of the wave and Δϕ\Delta \phi is the phase difference.

Complete Step by Step solution
A Quincke’s tube is an experimental setup that is used to demonstrate sound interference. A single sound source is passed on through one slit to divide and interfere before being detected at the other slit in the tube. Thus, interference is demonstrated by keeping one of the U tubes used in the experiment fixed and the other movable.
However, we know that the intensity of interference is given by I=I1+I2+2I1I2cosϕI = {I_1} + {I_2} + 2\sqrt {{I_1}{I_2}} \cos \phi . Also the maximum intensity of interference occurs at phase angle ϕ=0+2πn\phi = 0 + 2\pi n for any integer nn . Thus maximum intensity of interference is given by Imax=I1+I2+2I1I2cosϕ{I_{\max }} = {I_1} + {I_2} + 2\sqrt {{I_1}{I_2}} \cos \phi [since cos(0+2πn)=1\cos (0 + 2\pi n) = 1 ].
Given the maximum intensity Imax=I0{I_{\max }} = {I_0} and both the interfering waves have equal intensity I1=I2=I{I_1} = {I_2} = I , now rewriting the equation for maximum intensity of interference, I0=I+I+2I×Icos(0+2πn){I_0} = I + I + 2\sqrt {I \times I} \cos (0 + 2\pi n)
I0=2I+2I2(1)\Rightarrow {I_0} = 2I + 2\sqrt {{I^2}} (1)
Since cos(2πn)=1\cos (2\pi n) = 1 and I×I=I2I \times I = {I^2} . Simplifying the equation further we get,
I0=4I{I_0} = 4I
I04=I\Rightarrow \dfrac{{{I_0}}}{4} = I
Now we must find the intensity of interference for I02\dfrac{{{I_0}}}{2} . Rewriting the intensity equation with I=I02,I1=I04I = \dfrac{{{I_0}}}{2},{I_1} = \dfrac{{{I_0}}}{4} and I2=I04{I_2} = \dfrac{{{I_0}}}{4} we get,
I02=I04+I04+2I04I04cosϕ\dfrac{{{I_0}}}{2} = \dfrac{{{I_0}}}{4} + \dfrac{{{I_0}}}{4} + 2\sqrt {\dfrac{{{I_0}}}{4}\dfrac{{{I_0}}}{4}} \cos \phi
Simplifying the equation, we get,
I02=I0+I04+2I04I04cosϕ\Rightarrow \dfrac{{{I_0}}}{2} = \dfrac{{{I_0} + {I_0}}}{4} + 2\sqrt {\dfrac{{{I_0}}}{4}\dfrac{{{I_0}}}{4}} \cos \phi
I02=2I04+2I04I04cosϕ\Rightarrow \dfrac{{{I_0}}}{2} = \dfrac{{2{I_0}}}{4} + 2\sqrt {\dfrac{{{I_0}}}{4}\dfrac{{{I_0}}}{4}} \cos \phi
Taking 2I04\dfrac{{2{I_0}}}{4} to the L.H.S,
I022I04=2I02I04=2I04I04cosϕ\Rightarrow \dfrac{{{I_0}}}{2} - \dfrac{{2{I_0}}}{4} = \dfrac{{2{I_0} - 2{I_0}}}{4} = 2\sqrt {\dfrac{{{I_0}}}{4}\dfrac{{{I_0}}}{4}} \cos \phi [ taking L.C.M to the L.H.S]
0=2I04cosϕ\Rightarrow 0 = 2\dfrac{{{I_0}}}{4}\cos \phi [Since I04I04=I04\sqrt {\dfrac{{{I_0}}}{4}\dfrac{{{I_0}}}{4}} = \dfrac{{{I_0}}}{4} ]
So, now there can be two possibilities such that the R.H.S equates to 0, either I0=0{I_0} = 0 or cosϕ=0\cos \phi = 0 . However, I0=0{I_0} = 0 is not possible because it is the maximum intensity of interference. So, cosϕ=0\cos \phi = 0 .
cosϕ=0\cos \phi = 0 only when ϕ=π2\phi = \dfrac{\pi }{2} .
Δϕ=π20=π2\Rightarrow \Delta \phi = \dfrac{\pi }{2} - 0 = \dfrac{\pi }{2}
Using the phase difference Δϕ\Delta \phi we can find path difference by Δx=λ2π×π2\Delta x = \dfrac{\lambda }{{2\pi }} \times \dfrac{\pi }{2}
Δx=λ4\Rightarrow \Delta x = \dfrac{\lambda }{4}
Thus the minimum distance that the wave should travel to give intensity I02\dfrac{{{I_0}}}{2} is Δx=λ4\Delta x = \dfrac{\lambda }{4} .
So the correct answer is option B.

Note
The interference of the waves and its intensity are affected by a large factor when there is a change in the phase angle between the waves. Also here I1=I2=I{I_1} = {I_2} = I , hence the intensity is affected only by the phase angle ϕ\phi .