Waves

NEET Physics · 100 questions · Page 9 of 10 · Click an option or "Show Solution" to reveal answer

Q81
The displacement yy of a particle in a medium can be expressed as, y=106siny = {10^{ - 6}}\,\sin (100t+20x+π4)\left( {100t + 20x + {\pi \over 4}} \right) mm where tt is in second and xx in meter. The speed of the wave is
A 20m/s20\,\,m/s
B 5m/s5\,m/s
C 2000m/s2000\,m/s
D 5πm/s5\,\pi \,m/s
Correct Answer
Option B
Solution

From equation given,

ω=100\omega = 100

and

k=20,k = 20,
v=ωk=10020=5m/sv = {\omega \over k} = {{100} \over {20}} = 5m/s
Q82
If a wave gets refracted into a denser medium, then which of the following is true?
A wavelength, speed and frequency decreases.
B wavelength increases, sped decreases and frequency remains constant.
C wavelength and speed decreases but frequency remains constant.
D wavelength, speed and frequency increases.
Correct Answer
Option C
Solution

Frequency is independent of medium. For denser medium, wavelength and speed both would decrease.

Q83
A pipe of length 8585 cmcm is closed from one end. Find the number of possible natural oscillations of air column in the pipe whose frequencies lie below 12501250 HzHz. The velocity of sound in air is 340340 m/sm/s.
A 1212
B 88
C 66
D 44
Correct Answer
Option C
Solution

Length of pipe

=85=85
cmcm
=0.85m=0.85m

Pipe is closed from one end so it behaves as a closed organ pipe Frequency of oscillations of air column in closed organ pipe is given by,

f=(2n1)υ4Lf = {{\left( {2n - 1} \right)\upsilon } \over {4L}}
f=(2n1)υ4L1250f = {{\left( {2n - 1} \right)\upsilon } \over {4L}} \le 1250
(2n1)×3400.85×41250\Rightarrow {{\left( {2n - 1} \right) \times 340} \over {0.85 \times 4}} \le 1250
2n112.56\Rightarrow 2n - 1 \le 12.5 \approx 6

Possible value of n = 1, 2, 3, 4, 5, 6 So, number of possible natural frequencies lie below 1250 Hz is 6.

Q84
While measuring the speed of sound by performing a resonance column experiment, a student gets the first resonance condition at a column length of 1818 cmcm during winter. Repeating the same experiment during summer, she measures the column length to be xx cmcm for the second resonance. Then
A 18>x18 > x
B x>54x > 54
C 54>x>3654 > x > 36
D 36>x>1836 > x > 18
Correct Answer
Option B
Solution

For first resonant length

v=v41=v4×18v = {v \over {4{\ell _1}}} = {v \over {4 \times 18}}

(in winter) For second resonant length

v=3v42=3v4xv' = {{3v'} \over {4{\ell _2}}} = {{3v'} \over {4x}}

(in summer) \therefore

v4×18=3v4×x{v \over {4 \times 18}} = {{3v'} \over {4 \times x}}

\therefore

x=3×18×vvx = 3 \times 18 \times {{v'} \over v}

\therefore

x=54×vvcmx = 54 \times {{v'} \over v}cm
v>vv' > v

because velocity of light is greater in summer as compared to winter

(vT)\left( {v \propto \sqrt T } \right)

\therefore

x>54cmx > 54\,cm
Q85
Assume that the displacement(s) of air is proportional to the pressure difference (Δ\Delta p) created by a sound wave. Displacement (s) further depends on the speed of sound (v), density of air (ρ\rho ) and the frequency (f). If Δ\Delta p ~ 10 Pa, v ~ 300 m/s, ρ\rho ~ 1 kg/m3 and f ~ 1000 Hz, then s will be of the order of (take the multiplicative constant to be 1) :
A 1 mm
B 3100{3 \over {100}} mm
C 10 mm
D 110{1 \over {10}} mm
Correct Answer
Option B
Solution

Given, S \propto

Δ\Delta

p and Proportionally constant = 1 We know,

Δ\Delta

p = Sβ\betak = ρ\rhov2 ×\times

ωv×S{\omega \over v} \times S

=

ρvωS{\rho v\omega S}

\therefore S =

Δpρvω{{\Delta p} \over {\rho v\omega }}

=

Δpρv2πf{{\Delta p} \over {\rho v2\pi f}}

=

Δpρvf{{\Delta p} \over {\rho vf}}

[As Proportionally constant = 1 so assume 2π\pi = 1]

=101×300×1000= {{10} \over {1 \times 300 \times 1000}}
=130mm= {1 \over {30}}mm
3100mm\approx {3 \over {100}}mm
Q86
Two sitar strings, A and B, playing the note 'Dha' are slightly out of tune and produce beats of frequency 5 Hz. The tension of the string B s slightly increased and the beat frequency is found to decrease by 3Hz. If the frequency of A is 425 Hz, the original frequency of B is :
A 430 Hz
B 420 Hz
C 428 Hz
D 422 Hz
Correct Answer
Option B
Solution

Frequency of B, fB = 425 ±\pm 5 = 420 or 430 Hz As tension of string B is increased So, frequency of B, fB should also increase [as f \propto

T\sqrt T

] If initially fB = 430 Hz then when fB increases by increasing the tension then fB - fA increases that means beat frequency increase.

So, fB can't be 430 Hz When fB = 420 then when fB increases fA - fB decreases means beat frequency decreases.

So, correct fB = 420 Hz.

Q87
An observer moves towards a stationary source of sound with a velocity equal to one-fifth of the velocity of sound. The percentage change in the frequency will be :
A 20%
B 10%
C 5%
D 0%
Correct Answer
Option A
Solution
f=f0[vv0vvs]f' = {f_0}\left[ {{{v - {v_0}} \over {v - {v_s}}}} \right]
f=f0[v+v5v]\Rightarrow f' = {f_0}\left[ {{{v + {v \over 5}} \over v}} \right]
f=6f05\Rightarrow f' = {{6{f_0}} \over 5}

\Rightarrow % change = 20

Q88
Two engines pass each other moving in opposite directions with uniform speed of 30 m/s. One of them is blowing a whistle of frequency 540 Hz. Calculate the frequency heard by driver of second engine before they pass each other. Speed of sound is 330 m/sec :
A 450 Hz
B 540 Hz
C 648 Hz
D 270 Hz
Correct Answer
Option C
Solution

Frequency heard by the driver of second engine, F' =

(v+v0vvS)\left( {{{v + {v_0}} \over {v - {v_S}}}} \right)

f given v0 = vs = 30 m/s \therefore f' =

(330+3033030)×540\left( {{{330 + 30} \over {330 - 30}}} \right) \times 540

= 648 Hz

Q89
A granite rod of 60 cm length is clamped at its middle point and is set into longitudinal vibrations. The density of granite is 2.7 ×\times 103 kg/m3 and its Young’s modulus is 9.27 ×\times 1010 Pa. What will be the fundamental frequency of the longitudinal vibrations ?
A 7.5 kHz
B 5 kHz
C 2.5 kHz
D 10 kHz
Correct Answer
Option B
Solution

As rod length = 60 cm

\therefore\,\,\,
λ2{\lambda \over 2}

= 60 \Rightarrow

\,\,\,

λ\lambda = 120 cm = 1.2 m In solid, velocity of wave, V =

Yρ\sqrt {{Y \over \rho }}

=

9.27×10102.7×103\sqrt {{{9.27 \times {{10}^{10}}} \over {2.7 \times {{10}^3}}}}

= 5.85 ×\times 103 m/sec. As we know, v = f λ\lambda

\therefore\,\,\,

f =

vλ{v \over \lambda }

=

5.85×1031.2{{5.85 \times {{10}^3}} \over {1.2}}

= 4.88 ×\times 103 Hz

\simeq

5 kHz

Q90
A sound absorber attenuates the sound level by 2020 dBdB. The intensity decreases by a factor of
A 100100
B 10001000
C 1000010000
D 1010
Correct Answer
Option A
Solution

We have,

L1=10log(I1I0);{L_1} = 10\log \left( {{{{{\rm I}_1}} \over {{{\rm I}_0}}}} \right);
L2=10log(I2I0){L_2} = 10\,\log \left( {{{{{\rm I}_2}} \over {{{\rm I}_0}}}} \right)

\therefore

L1L2=10log(I1I0)10log(I2I0)\,\,{L_1} - {L_2} = 10\,\log \left( {{{{{\rm I}_1}} \over {{{\rm I}_0}}}} \right) - 10\,\log \left( {{{{{\rm I}_2}} \over {{{\rm I}_0}}}} \right)

or,

ΔL=10log(I1I0×I0I2)\Delta L = 10\,\log \left( {{{{{\rm I}_1}} \over {{{\rm I}_0}}} \times {{{{\rm I}_0}} \over {{{\rm I}_2}}}} \right)

or,

ΔL=10log(I1I2)\Delta L = 10\,\log \left( {{{{{\rm I}_1}} \over {{{\rm I}_2}}}} \right)

or,

20=10log(I1I2)20 = 10\log \left( {{{{{\rm I}_1}} \over {{{\rm I}_2}}}} \right)

or,

2=log(I1I2)2 = \log \left( {{{{{\rm I}_1}} \over {{{\rm I}_2}}}} \right)

or,

I1I2=102{{{{\rm I}_1}} \over {{{\rm I}_2}}} = {10^2}

or,

I2=I1100.{{\rm I}_2} = {{{{\rm I}_1}} \over {100}}.

\Rightarrow Intensity decreases by a factor

100.100.
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