Waves

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

Q91
A stationary observer receives sound from two identical tuning forks, one of which approaches and the other one recedes with the same speed (much less than the speed of sound). The observer hears 2 beats/sec. The oscillation frequency of each tuning fork is v0 = 1400 Hz and the velocity of sound in air is 350 m/s. The speed of each tuning fork is close to :
A 1 m/s
B 18{1 \over 8} m/s
C 14{1 \over 4} m/s
D 12{1 \over 2} m/s
Correct Answer
Option C
Solution

f1 =

(ccv)f0\left( {{c \over {c - v}}} \right){f_0}

f1 =

(cc+v)f0\left( {{c \over {c + v}}} \right){f_0}

beat frequency = f1 – f2 =

cf0(1cv1c+v)c{f_0}\left( {{1 \over {c - v}} - {1 \over {c + v}}} \right)

=

cf0(2vc2v2)c{f_0}\left( {{{2v} \over {{c^2} - {v^2}}}} \right)

As c \gg v then

c2v2{{c^2} - {v^2}}

=

c2{{c^2}}

=

cf0(2vc2)c{f_0}\left( {{{2v} \over {{c^2}}}} \right)

=

f0(2vc){f_0}\left( {{{2v} \over c}} \right)

\therefore

f0(2vc){f_0}\left( {{{2v} \over c}} \right)

= 2 \Rightarrow v =

3501400{{350} \over {1400}}

=

14{1 \over 4}

m/s

Q92
A tuning fork vibrates with frequency 256256 HzHz and gives one beat per second with the third normal mode of vibration of an open pipe. What is the length of the pipe ? (Speed of sound in air is 340ms1340\,m{s^{ - 1}})
A 220220 cmcm
B 190190 cmcm
C 180180 cmcm
D 200200 cmcm
Correct Answer
Option D
Solution

The tuning fork vibrates with frequency 256 Hz and give one beat per second So, the organ pipe will have frequency (256 ±\pm 1) Hr.

For open organ pipe, Frequency n =

Nυ2{{N\upsilon } \over {2\ell }}

Here n = 255 Hz N = 3

υ\upsilon

= 340 m/s

\therefore\,\,\,\,

255 =

3×3402×{{3 \times 340} \over {2 \times \ell }}

\Rightarrow

\,\,\,\,
\ell

=

3×3402×255=2m{{3 \times 340} \over {2 \times 255}} = 2\,m
\therefore\,\,\,\,
\ell

= 2m or 200 cm

Q93
The equation of a transverse wave travelling along a string is y(x,t)=4.0sin[20×103x+600t]mmy(x, t)=4.0 \sin \left[20 \times 10^{-3} x+600 t\right] \mathrm{mm}, where xx is in mm and tt is in second. The velocity of the wave is :
A 60 m/s-60 \mathrm{~m} / \mathrm{s}
B +60 m/s+60 \mathrm{~m} / \mathrm{s}
C +30 m/s+30 \mathrm{~m} / \mathrm{s}
D 30 m/s-30 \mathrm{~m} / \mathrm{s}
Correct Answer
Option D
Solution

Let's analyze the wave equation step by step. The given wave is:

y(x,t)=4.0sin[20×103x+600t] mm.y(x, t) = 4.0 \sin \left[20 \times 10^{-3} x + 600 t\right] \text{ mm}.

First, simplify the coefficient of x x :

20×103=0.02mm1.20 \times 10^{-3} = 0.02 \, \text{mm}^{-1}.

So the equation becomes:

y(x,t)=4.0sin(0.02x+600t) mm.y(x, t) = 4.0 \sin\left(0.02x + 600t\right) \text{ mm}.

A standard form for a travelling wave is:

y(x,t)=Asin(kxωt)y(x, t) = A \sin(kx - \omega t)

which represents a wave moving in the positive x x -direction with speed v=ωk v = \dfrac{\omega}{k} .

Notice that our wave equation has the form:

sin(0.02x+600t)\sin(0.02x + 600t)

The positive sign in front of 600t 600t means we can rewrite the phase as:

0.02x+600t=0.02x(600t),0.02x + 600t = 0.02x - (-600t),

which indicates that the angular frequency ω \omega in the standard form is effectively 600 -600 .

The velocity v v of a wave is determined from the phase (for a constant phase, ϕ= \phi = constant):

kx+ωt=constant.k x + \omega t = \text{constant}.

Differentiating with respect to t t :

kdxdt+ω=0,k \frac{dx}{dt} + \omega = 0,

which gives:

dxdt=ωk.\frac{dx}{dt} = -\frac{\omega}{k}.

Substituting the values: k=0.02mm1 k = 0.02 \, \text{mm}^{-1} ω=600s1 \omega = 600 \, \text{s}^{-1} We have:

v=6000.02=30000 mm/s.v = -\frac{600}{0.02} = -30000 \text{ mm/s}.

Convert the velocity from mm/s to m/s:

30000mm/s=30m/s.-30000 \, \text{mm/s} = -30 \, \text{m/s}.

Thus, the velocity of the wave is 30m/s-30 \, \text{m/s}. The correct answer is Option D.

Q94
Two cars A and B are moving away from each other in opposite directions. Both the cars are moving with a speed of 20 ms–1 with respect to the ground. If an observer in car A detects a frequency 2000 Hz of the sound coming from car B, what is the natural frequency of the sound source in car B ? (speed of sound in air = 340 ms–1) :-
A 2300 Hz
B 2060 Hz
C 2250 Hz
D 2150 Hz
Correct Answer
Option C
Solution
f=(v±u0)(v±us).f0=(v20)(v+20).f0f = {{\left( {v \pm {u_0}} \right)} \over {\left( {v \pm {u_s}} \right)}}.{f_0} = {{\left( {v - 20} \right)} \over {\left( {v + 20} \right)}}.{f_0}
2000=320360.f0\Rightarrow 2000 = {{320} \over {360}}.{f_0}
2000×98=f0=2250Hz\Rightarrow {{2000 \times 9} \over 8} = {f_0} = 2250\,Hz
Q95
Two strings with circular cross section and made of same material, are stretched to have same amount of tension. A transverse wave is then made to pass through both the strings. The velocity of the wave in the first string having the radius of cross section R is v1v_1, and that in the other string having radius of cross section R/2 is v2v_2. Then v2v1\dfrac{v_2}{v_1} =
A 8
B 4
C 2
D 2\sqrt{2}
Correct Answer
Option C
Solution

To find the ratio of the velocities of transverse waves in two strings with different radii but identical materials and tension, consider the following: The wave velocity v v in a string is given by the formula: v=Tμ v = \sqrt{\dfrac{T}{\mu}} where T T is the tension and μ \mu is the linear mass density of the string, defined as: μ=ρπR2 \mu = \rho \pi R^2 Here, ρ \rho is the density of the material, and R R is the radius of the string.

Given that both strings have the same tension T T and material, we compare their wave velocities v1 v_1 and v2 v_2 for radii R1=R R_1 = R and R2=R2 R_2 = \dfrac{R}{2} .

The velocity ratio is expressed as: v2v1=TρπR22TρπR12 \dfrac{v_2}{v_1} = \dfrac{\sqrt{\dfrac{T}{\rho \pi R_2^2}}}{\sqrt{\dfrac{T}{\rho \pi R_1^2}}} Simplifying this expression: v2v1=R12R22=R1R2=RR2=2 \dfrac{v_2}{v_1} = \dfrac{\sqrt{R_1^2}}{\sqrt{R_2^2}} = \dfrac{R_1}{R_2} = \dfrac{R}{\dfrac{R}{2}} = 2 Thus, the ratio v2v1 \dfrac{v_2}{v_1} is 2.

Q96
Tube AA has bolt ends open while tube BB has one end closed, otherwise they are identical. The ratio of fundamental frequency of tube AA and BB is
A 1:21:2
B 1:41:4
C 2:12:1
D 4:14:1
Correct Answer
Option C
Solution

KEY CONCEPT : The fundamental frequency for closed organ pipe is given by

υc=v4{\upsilon _c} = {v \over {4\ell }}

and For open organ pipe is given by

υ0=v2{\upsilon _0} = {v \over {2\ell }}

\therefore

υ0υc=v2×4v=21{{{\upsilon _0}} \over {{\upsilon _c}}} = {v \over {2\ell }} \times {{4\ell } \over v} = {2 \over 1}
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