Solved Examples on Waves & Sound Waves

Question 1:-A sound wave of 42.0-cm wavelength enters the tube shown in the below figure. What must be the smallest radiusrsuch that a minimum will be heard at the detector?

Concept:A minimum sound will be heard at the detector if the sound waves coming from the curve part and the straight part is equal to the half the wavelength of the sound waves.

Solution:The corresponding figure of the sound waves in the passing through the curve part and straight part is shown below:

Consider the sound waves start from the point

A. The sound waves will meet at the pointBand interfere and can be detected.The path length of the sound waves passing through the curve is equal to half the circle having radius

rcentered atC.Thus, the path length of the sound waves in the curve part is

L_{1}=πrThe path length of the sound in the tube

ABCis equal to the diameter of the circle having radiusrcentered atC. So, the path length of the sound waves traveling in it is

L_{2}=2rNow, the path difference of the sound waves at the point

CisΔ

p=L_{1}-L_{2}= π

r– 2r= (π – 2)

rFor the sound to be heard minimum at the detector, the difference in path length of the sound waves is

Δ

p=λ/2Insert Δ

p= (π – 2)rin the above equation givesΔ

p=λ/2(π – 2)

r=λ/2

r=λ/[2(π-2)]Substitute 42.0 cm for

λin the above equation gives

r=λ/[2(π-2)]= [(42.0 cm) (10

^{-2}m/1 cm)]/2(3.14-2)= 18.421×10

^{-2}mRounding off to three significant figures, the smallest radius of the curve part of the tube to be heard minimum sound at the detector is 18.4×10

^{-2}m.

Question 2:- Two stereo loud speakers are separated by a distance of 2.12 m. Assume that the amplitude of the sound from each speaker is approximately the same at the position of a listener, who is 3.75 m directly in front one of the speakers; see below figure.(a)For what frequencies in the audible range (20-20,000 Hz) will there be a minimum signal?(b)For what frequencies is the sound a maximum?

Concept:The signal observed will be minimum when the path difference between the signals from the sources is equal to half integral multiple of the wavelength.

The signal observed will be maximum when the path difference between the signals from the sources is equal to the integral multiple of the wavelength.

Solution:

(a)The corresponding figure for the signals coming from the sources is shown below:

From the figures, the two speaker are labeled asS_{1}andS_{2}. The listener is labeled asO.From the triangle

S_{1}S_{2}O, the pathS_{1}Ois

S_{1}O= √[(S_{1}S_{2})^{2}+ (S_{2}O)^{2}]= √[(2.12 m)

^{2}+ (3.75 m)^{2}]= 4.3078 m

Now, the path difference between the signal coming from the speakers

S_{1}andS_{2}isΔ

p=S_{1}O-S_{2}O= 4.31 m – 3.75 m

= 0.56 m

The signal observed by the listener will be minimum when the path difference is equal to the half integral multiple of the wavelength

λ.Δ

p= (n- ½ )λHere,

n= 1,2,3….The wavelength of the sound wave is

λ=v/fHere, speed of the sound waves is and frequency of the sound wave is

f.Insert

λ=v/fin the equation Δp= (n- ½ )λgivesΔ

p= (n- ½ )λ= (

n- ½ ) (v/f)

f= (n- ½ ) (v/Δp)The speed of the sound waves in air at room temperature is 343 m/s.

Substitute 343 m/s for

vand 0.56 m for Δpin the equationf= (n- ½ ) (v/Δp) gives

f= (n- ½ ) (v/Δp)= (

n- ½ ) [(343 m/s)/(0.56 m)] (1 Hz.s)= (

n– ½) 612.5 HzRounding off to three significant figures, the frequencies of the speakers should

(

n– ½) 613 Hz for the single to be minimum.

(b)The signal observed by the listener will be maximum when the path difference is equal to the integral multiple of the wavelengthλ.Δ

p=nλHere,

n= 1,2,3…..The wavelength of the sound wave is

λ=v/fHere, speed of the sound waves is

vand frequency of the sound wave isf.Insert

λ=v/fin the equation Δp=nλgivesΔ

p=nλ=

n(v/f)

f=n(v/ Δp)The speed of the sound waves in air at room temperature is 343 m/s.

Substitute 343 m/s for

vand 0.56 m for Δpin the equationf=n(v/ Δp), gives

f=n(v/ Δp)=

n[(343 m/s)/(0.56 m)] (1 Hz.s)=

n(612.5 Hz)Rounding off to three significant figures, the frequencies of the speakers should

n(613 Hz) for the single to be maximum.

Question 3:-Sin below figure is a small loudspeaker driven by an audio oscillator and amplifier, adjustable in frequency from 1000 to 2000 Hz only.Dis a piece of cylindrical sheet metal pipe 45.7 cm long and opens at both ends. (a) At what frequencies will resonance occur when the frequency emitted by the speaker is varied from 1000 to 2000 Hz? (b) Sketch the displacement nodes for each resonance. Neglect end effects.

Concept:The given cylindrical sheet metal pipe is equivalent to open tube pipes.

The resonant frequency of the open tube pipe is

f=_{n}n(v/2L)Here,

n= 1,2,3…..., speed of the sound in the tube isvand length of the tube isL.For corresponding frequencies emitted by the small loudspeaker, the tube will resonate.

Solution:

(a)The speed of the sound in air at room temperature is 343 m/s.Substitute 343 m/s for

vand 45.7 cm for in the equationf=_{n}n(v/2L) gives

f=_{n}n[v/2L]=

n[ (343 m/s)/2 (45.7 cm) (10^{-2}m/1 cm)]=

n(375.275/s) (1 Hz.s)=

n(375.275 Hz)

For the first harmonic, insertn= 1 in the equationf=_{n}n(375.275 Hz)gives

f=_{n}n(375.275 Hz)

f_{1}= (1) (375.275 Hz)= 375.275 Hz

For the second harmonic, insert

n= 2 in the equationf=_{n}n(375.275 Hz) gives

f_{2}= (2) (375.275 Hz)= 750.55 Hz

For the third harmonic, insert

n= 3 in the equationf=_{n}n(375.275 Hz) gives

f_{3}= (3) (375.275 Hz)= 1125.825 Hz

For the fourth harmonic, insert

n= 4 in the equationf=_{n}n(375.275 Hz) gives

f_{4}= (4) (375.275 Hz)= 1501.1 Hz

For the fifth harmonic, insert

n= 5 in the equationf=_{n}n(375.275 Hz) gives

f_{5}= (5) (375.275 Hz)= 1876.375 Hz

For the sixth harmonic, insert

n= 6 in the equationf=_{n}n(375.275 Hz) gives

f_{6}= (6) (375.275 Hz)= 2251.65 Hz

It is given that the frequency emitted by the small loudspeaker is varied from 1000 Hz to 2000 Hz. This means the tube will oscillate with frequencies lies between 1000 Hz to 2000 Hz. So, the first, second and sixth harmonics are not resonating with the tube as their frequencies leis beyond the given range. Only third, fourth and fifth harmonic will resonate.

Rounding off to three significant figures, the tube will resonate at frequencies 1130 Hz, 1500 Hz, and 1880 Hz.

(b)Forn= 3, the displacement nodes are shown below:

Forn= 4, the displacement nodes are shown below:

Forn= 5, the displacement nodes are shown below: