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Question: The ratio of intensities of two waves are given by \(4:1\) . Then the ratio of the amplitude of the ...

The ratio of intensities of two waves are given by 4:14:1 . Then the ratio of the amplitude of the two waves is :
(A) 2:12:1
(B) 1:21:2
(C) 4:14:1
(D) 1:41:4

Explanation

Solution

Hint the intensity and amplitude are related to each other by square law. We will use that formula to calculate the ratio of amplitudes.

Complete Step-by-step Solution
The formula of intensity is given by energy per unit area per unit time.
\Rightarrow I=EAr×tI = \dfrac{E}{{Ar \times t}} ……(i)
Where I=I = intensity of wave
\Rightarrow E=E = energy of wave
\Rightarrow Ar=Ar = area on which it is falling
\Rightarrow t=t = time in seconds.
Eq (i) can be rewritten as –
\Rightarrow I=PArI = \dfrac{P}{{Ar}} …….(ii)
We will now calculate power and area to see the relation between amplitude and intensity.

Let the equation of the wave be given as:
\Rightarrow y=Asin(ωtkx)y = A\sin (\omega t - kx)
The energy per unit length of this wave is determined experimentally and is given by:
\Rightarrow dEdx=μA2ω2cos2(ωtkx)\dfrac{{dE}}{{dx}} = \mu {A^2}{\omega ^2}{\cos ^2}(\omega t - kx)
The power of the wave is given by-
P=energytime P=dEdt×dxdx P=v×dEdx P=vA2ω2μcos2(ωtkx)   P = \dfrac{{energy}}{{time}} \\\ P = \dfrac{{dE}}{{dt}} \times \dfrac{{dx}}{{dx}} \\\ P = v \times \dfrac{{dE}}{{dx}} \\\ P = v{A^2}{\omega ^2}\mu {\cos ^2}(\omega t - kx) \\\ \\\
In one frequency , the power travelled is average power.
\Rightarrow Pavg=1A2ω2μv2{P_{avg}} = \dfrac{{1{A^2}{\omega ^2}\mu v}}{2}
In eq (ii) , we will use average power as the value of power.
Now coming to eq (ii)-
I=PAr I=A2ω2μv2Ar   I = \dfrac{P}{{Ar}} \\\ I = \dfrac{{{A^2}{\omega ^2}\mu v}}{{2Ar}} \\\ \\\
Where
A=A = amplitude of wave
\Rightarrow μ=\mu = mass per unit length
\Rightarrow ω=\omega = angular frequency
\Rightarrow v=v = velocity of wave
μ=mL\mu = \dfrac{m}{L} putting this in the formula of intensity .
m=m = mass of the string in which the wave is travelling
L=L = length of the string in which the wave is travelling.
\Rightarrow I=12×A2ω2mVv I=12A2ω2vρ I=12A2(2πf)2vρ I=2A2π2f2ρv  I = \dfrac{1}{2} \times {A^2}{\omega ^2}\dfrac{m}{V}v \\\ I = \dfrac{1}{2}{A^2}{\omega ^2}v\rho \\\ I = \dfrac{1}{2}{A^2}{(2\pi f)^2}v\rho \\\ I = 2{A^2}{\pi ^2}{f^2}\rho v \\\
This is the derived formula of intensity . We can clearly see that-
IA2I \propto {A^2}
\Rightarrow I1I2=A12A22 A1A2=I1I2 A1A2=41 A1A2=21  \dfrac{{{I_1}}}{{{I_2}}} = \dfrac{{A_1^2}}{{A_2^2}} \\\ \dfrac{{{A_1}}}{{{A_2}}} = \sqrt {\dfrac{{{I_1}}}{{{I_2}}}} \\\ \dfrac{{{A_1}}}{{{A_2}}} = \sqrt {\dfrac{4}{1}} \\\ \dfrac{{{A_1}}}{{{A_2}}} = \dfrac{2}{1} \\\

Hence the correct option is A.

Note We have considered a wave travelling in a string here. The string has certain mass and length and that is what mm and LL are.