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Question: A friend rides, in turn, the rims of three fast merry-go-roundswhile holding a sound source that emits isotropically at a certain frequency. You stand far from each merry-go-round. The frequency you hear for each of your friend’s three rides varies as the merry-go-round rotates. The variations in frequency for the three rides aregiven by the three curves in Fig. 17-29. Rank the curves according to:

(a) the linear speed vof the sound source, (b) the angular speedsvofthe merry-go-rounds, and (c) the radii rof the merry-go-rounds, greatest first

Short Answer

Expert verified

Answer

  1. The ranks of the curves according to the linear speedof the sound are

Curve 3 > Curve 2 = Curve 1.

  1. The ranks of the curves according to the angular speed ωof the merry-go-rounds areCurve 1 > Curve 2 = Curve 1.
  2. The ranks of the curves according to the radiiof the merry-go-rounds are

Curve 3 > Curve 2 > Curve 1.

Step by step solution

01

Step 1: Stating given data

See Figure 17-29

02

Determining the concept

By using the formulae for the speed vof sound, the angular frequency ωand thelinear speed v, find theranks of the curves according to the linear speed vof the sound,according to the angular speed ωof the merry-go-rounds, and according to the radii rof the merry-go-rounds.

The formulae are as follows:

  1. The speedof sound is

v=fλ

2.The angular frequency ω is

ω=2πT

3.The linear speed is

v=rω

where f is frequency, r is radius, ω is an angular frequency,λ is wavelength, T is time and vis velocity

03

(a) Determining the ranks of the curves according to the linear speed of vof the sound

From the Doppler Effect, the apparent frequency of the source of sound would be maximum when the velocity of the source approaching towards it is the maximum. As seen in the graph, the apparent frequency of sound for 3rdmerry-go is highest and it is same for the 1st and the 2nd. So, the linear velocity of the source on the 3rdmerry-go round would be higher and the same goes for the 1st and the 2nd.

04

(b) Determining the ranks of the curves according to the angular speed ω of the merry-go-rounds

The time taken by the merry-go-round to complete one rotation would be equivalent to the time period of one complete wave shown in the graph. As angular velocity is inversely proportional to the time period, we can conclude that the 1st one would have highest angular velocity, as the wave has the smallest time period out of all the waves. The angular velocity of the 2nd and the 3rd would be the same and smaller than that of the 1st., because they have the same time period which is greater than that of the 1st wave. Therefore, we can write

1 > 2 =3

05

(c) Determining the ranks of the curves according to the radii r of the merry-go-rounds

Linear velocity of the merry-go-round can be written as

v=rω

Therefore

r1=v1ω1r2=v2ω2r3=v3ω3

From the first two cases, it is clear that the linear velocity of the 1st is the greatest and the angular velocity is the smallest. Using this, it can be concluded that the radius would be the largest for the 3rd.

The linear velocity of the 1st and 2nd is the same. So, the radius value for these two would be inversely proportional to the angular velocity. Now, from the second case, the angular velocity of the 1st is greater than the angular velocity of the 2nd. Therefore, the radius of the 1st would be smaller than that of the 2nd. From this, the 3rd has the largest radius, followed by the 2nd, and the 1st would have the smallest radius; that is, 3>2>1.

Thus, by using the formulae for the speed of sound, the angular frequency ω and the linear speed , the answer to this question can be found.

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Most popular questions from this chapter

Party hearing. As the number of people at a party increases, you must raise your voice for a listener to hear you against the background noise of the other partygoers. However, once you reach the level of yelling, the only way you can be heard is if you move closer to your listener, into the listener’s “personal space.” Model the situation by replacing you with an isotropic point source of fixed power P and replacing your listener with a point that absorbs part of your sound waves. These points are initially separated byri=1.20 m . If the background noise increases byΔβ=5dB , the sound level at your listener must also increase. What separationrf is then required?

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