Waves

JEE Physics · 96 questions · Page 6 of 10 · Click an option or "Show Solution" to reveal answer

Q51
A longitudinal wave is represented by x=10sin2π(ntxλ)x = 10\sin 2\pi \left( {nt - {x \over \lambda }} \right) cm. The maximum particle velocity will be four times the wave velocity if the determined value of wavelength is equal to :
A 2π\pi
B 5π\pi
C π\pi
D 5π2{{5\pi } \over 2}
Correct Answer
Option B
Solution

Particle velocity =

xt{{\partial x} \over {\partial t}}

\Rightarrow Maximum particle velocity

=(2πn)(10)= (2\pi n)\,(10)
(2πn)(10)=(nλ)(4)\Rightarrow (2\pi n)\,(10) = (n\lambda )\,(4)
λ=5π\Rightarrow \lambda = 5\pi
Q52
The equations of two waves are given by : y1 = 5 sin 2π\pi(x - vt) cm y2 = 3 sin 2π\pi(x - vt + 1.5) cm These waves are simultaneously passing through a string. The amplitude of the resulting wave is :
A 2 cm
B 4 cm
C 5.8 cm
D 8 cm
Correct Answer
Option A
Solution
y1=5sin(2πx2πvt){y_1} = 5\sin (2\pi x - 2\pi vt)
y2=3sin(2πx2πvt+3π){y_2} = 3\sin (2\pi x - 2\pi vt + 3\pi )

\Rightarrow Phase difference = 3π\pi

Anet=A12+A22+2A1A2cos(3π)\Rightarrow {A_{net}} = \sqrt {A_1^2 + A_2^2 + 2{A_1}{A_2}\cos (3\pi )}
Anet=2\Rightarrow {A_{net}} = 2

cm

Q53
Which of the following equations correctly represents a travelling wave having wavelength λ\lambda = 4.0 cm, frequency v = 100 Hz and travelling in positive x-axis direction?
A y=Asin[(0.50πcm1)x(100πs1)t]y = A\sin [(0.50\,\pi \,c{m^{ - 1}})x - (100\,\pi \,{s^{ - 1}})t]
B y=Asin2π[(0.25cm1)x(50s1)t]y = A\sin \,\,2\pi [(0.25\,\,c{m^{ - 1}})x - (50\,{s^{ - 1}})t]
C y=Asin[(2π4cm1)x(2π100s1)t]y = A\sin \left[ {\left( {{{2\pi } \over 4}\,c{m^{ - 1}}} \right)x - \left( {{{2\pi } \over {100}}\,{s^{ - 1}}} \right)t} \right]
D y=Asinπ[(0.5cm1)x(200s1)t]y = A\sin \,\pi [(0.5\,\,c{m^{ - 1}})x - (200\,\,{s^{ - 1}})t]
Correct Answer
Option D
Solution

We know, equation of wave travelling in positive x-direction is -

y=Asin(kxwt)y = A\sin (kx - wt)

where

k=2πλk = {{2\pi } \over \lambda }

and

w=2πfw = 2\pi f

Here given λ\lambda = 4 cm and frequency (f) = 100 Hz \therefore

k=2π4=0.5πk = {{2\pi } \over 4} = 0.5\pi

cm-1 and

w=2π×100=200πw = 2\pi \times 100 = 200\pi

s-1 \therefore Equation of travelling wave,

y=Asin(0.5πx200πt)y = A\sin (0.5\pi x - 200\pi t)
Q54
A transverse wave is represented by y=2sin(ωtkx)cmy=2 \sin (\omega t-k x)\, \mathrm{cm}. The value of wavelength (in cm\mathrm{cm}) for which the wave velocity becomes equal to the maximum particle velocity, will be :
A 4π\pi
B 2π\pi
C π\pi
D 2
Correct Answer
Option A
Solution
ωk=Aω{\omega \over k} = A\omega
k=1A=12cm\Rightarrow k = {1 \over A} = {1 \over {2\,cm}}
2πλ=12cm\Rightarrow {{2\pi } \over \lambda } = {1 \over {2\,cm}}
λ=4πcm\Rightarrow \lambda = 4\pi \,cm
Q55
In the wave equation y=0.5sin2πλ(400tx)m y=0.5 \sin \dfrac{2 \pi}{\lambda}(400 \mathrm{t}-x) \,\mathrm{m} the velocity of the wave will be:
A 200 m/s
B 2002\sqrt2 m/s
C 400 m/s
D 4002\sqrt2 m/s
Correct Answer
Option C
Solution
vwave=coefficientoftcoefficientofx{v_{wave}} = \left| {{{coefficient\,of\,t} \over {coefficient\,of\,x}}} \right|
=4001=400= {{400} \over 1} = 400

m/s

Q56
A steel wire with mass per unit length 7.0×103 kg m17.0 \times 10^{-3} \mathrm{~kg} \mathrm{~m}^{-1} is under tension of 70 N70 \mathrm{~N}. The speed of transverse waves in the wire will be:
A 10 m/s10 \mathrm{~m} / \mathrm{s}
B 50 m/s50 \mathrm{~m} / \mathrm{s}
C 100 m/s100 \mathrm{~m} / \mathrm{s}
D 200π m/s200 \pi\mathrm{~m} / \mathrm{s}
Correct Answer
Option C
Solution

Speed of transverse wave =Tμ=\sqrt{\dfrac{T}{\mu}} =707×103=100 m/s=\sqrt{\dfrac{70}{7 \times 10^{-3}}}=100 \mathrm{~m} / \mathrm{s}

Q57
A person observes two moving trains, 'A' reaching the station and 'B' leaving the station with equal speed of 30 m/s30 \mathrm{~m} / \mathrm{s}. If both trains emit sounds with frequency 300 Hz300 \mathrm{~Hz}, (Speed of sound: 330 m/s330 \mathrm{~m} / \mathrm{s}) approximate difference of frequencies heard by the person will be:
A 10 Hz
B 55 Hz
C 80 Hz
D 33 Hz
Correct Answer
Option B
Solution

By doppler effect : f=f0[vv0vvs]f^{\prime}=f_{0}\left[\dfrac{v-v_{0}}{v-v_{s}}\right] fA=300[33033030]Hz\Rightarrow \quad f_{A}^{\prime}=300\left[\dfrac{330}{330-30}\right] \mathrm{Hz}

=330 Hz=330 \mathrm{~Hz}

And fB=300[330330+30]Hzf_{B}^{\prime}=300\left[\dfrac{330}{330+30}\right] \mathrm{Hz}

=56×330 Hz=275 Hz=\frac{5}{6} \times 330 \mathrm{~Hz}=275 \mathrm{~Hz}

Δf=330275=55 Hz\therefore \Delta \mathrm{f}=330-275=55 \mathrm{~Hz}.

Q58
A car P travelling at 20 ms120 \mathrm{~ms}^{-1} sounds its horn at a frequency of 400 Hz400 \mathrm{~Hz}. Another car Q\mathrm{Q} is travelling behind the first car in the same direction with a velocity 40 ms140 \mathrm{~ms}^{-1}. The frequency heard by the passenger of the car Q\mathrm{Q} is approximately [Take, velocity of sound =360 ms1=360 \mathrm{~ms}^{-1} ]
A 485 Hz
B 514 Hz
C 421 Hz
D 471 Hz
Correct Answer
Option C
Solution

Using the Doppler effect formula:

f=f0(c+v0c+vs)f = f_0\left(\frac{c + v_0}{c + v_s}\right)

where

ff

is the observed frequency (frequency heard by the passenger in car Q)

f0f_0

is the source frequency (400 Hz)

cc

is the speed of sound (360 m/s)

v0v_0

is the velocity of the observer (passenger in car Q) relative to the medium (air) in the direction of the source (40 m/s)

vsv_s

is the velocity of the source (car P) relative to the medium (air) in the direction of the observer (20 m/s, since it's moving in the same direction as car Q) Plugging in the values:

f=400(360+40360+20)f = 400\left(\frac{360 + 40}{360 + 20}\right)
f=400(400380)f = 400\left(\frac{400}{380}\right)
f=421f = 421

So, the observed frequency is 421 Hz.

Q59
For a periodic motion represented by the equation y=sinωt+cosωty=\sin \omega \mathrm{t}+\cos \omega \mathrm{t} the amplitude of the motion is
A 1
B 2\sqrt2
C 0.5
D 2
Correct Answer
Option B
Solution

We can write the given equation as:

y=(sinωt)2+(cosωt)2cos(ωtarctansinωtcosωt)y = \sqrt{(\sin\omega t)^2 + (\cos\omega t)^2} \cos\left(\omega t - \arctan\frac{\sin\omega t}{\cos\omega t}\right)

Using the identity sin2θ+cos2θ=1\sin^2\theta + \cos^2\theta = 1, we get:

y=1+sin2ωtcos(ωtπ4)y = \sqrt{1 + \sin 2\omega t} \cos\left(\omega t - \frac{\pi}{4}\right)

The amplitude of the motion is the maximum value of y|y|, which occurs when sin2ωt=1\sin 2\omega t = 1, i.e., at t=π4ω+nπωt = \dfrac{\pi}{4\omega} + \dfrac{n\pi}{\omega}, where nn is an integer.

Substituting this value of tt in the above equation, we get:

ymax=1+sinπ2=2|y_{\text{max}}| = \sqrt{1 + \sin \frac{\pi}{2}} = \sqrt{2}

Therefore, the amplitude of the motion is 2\sqrt{2}

Q60
The engine of a train moving with speed 10 ms110 \mathrm{~ms}^{-1} towards a platform sounds a whistle at frequency 400 Hz400 \mathrm{~Hz}. The frequency heard by a passenger inside the train is: (neglect air speed. Speed of sound in air =330 ms1=330 \mathrm{~ms}^{-1} )
A 200 Hz
B 412 Hz
C 400 Hz
D 388 Hz
Correct Answer
Option C
Solution

The phenomenon of frequency change due to relative motion between a source and an observer is called Doppler effect.

However, if the observer is at rest relative to the source (as in this case where the passenger is inside the train), then the frequency heard by the observer is the same as the frequency produced by the source.

This is because the relative velocity between the source (whistle) and the observer (passenger in the train) is zero.

The Doppler effect only applies when there is a relative velocity between the source and the observer.

Therefore, the frequency heard by the passenger inside the train is the same as the frequency of the whistle, i.e., 400 Hz.

So, the correct answer is: 400 Hz.

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