chapter 12 sound ass/sound/soundtoc. html · pdf file · 2014-06-28chapter 12 sound...

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1 CHAPTER 12 SOUND http://www.physicsclassroom.com/Cl ass/sound/soundtoc. html Characteristics of Sound Intensity of Sound: Decibels The Ear and Its Response; Loudness Sources of Sound: Vibrating Strings and Air Columns Quality of Sound, and Noise; Superposition Interference of Sound Waves; Beats Doppler Effect Shock Waves and the Sonic Boom Characteristics of Sound Sound can travel through any kind of matter, but not through a vacuum. The speed of sound is different in different materials; in general, it is slowest in gases, faster in liquids, and fastest in solids. The speed depends somewhat on temperature, especially for gases. The speed of sound in air at and 1 atm, is 331 m/s. The speed increases approximately 0.60 m/s for each Celsius degree increase in temperature. Unless stated otherwise, assume that the temperature will be: Loudness: related to intensity of the sound wave Pitch: related to frequency. Audible range: about 20 Hz to 20,000 Hz; upper limit decreases with age Ultrasound: above 20,000 Hz; Infrasound: below 20 Hz There are three aspects of any sound: 1. There must be a source for a sound; and as with any wave, the source of a sound must be a vibrating object. 2. The energy is transferred from the source in the form of longitudinal sound waves 3. The sound is detected by an ear or an instrument 0 o C (331 0.60 ) / v Tms 20 , so [331 (0.60)(20 )] 343 / o o C v C ms

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Page 1: CHAPTER 12 SOUND ass/sound/soundtoc. html · PDF file · 2014-06-28CHAPTER 12 SOUND ass/sound/soundtoc. html ... So why does a trumpet sound different from a flute? The answer lies

1

CHAPTER 12 SOUND

http://www.physicsclassroom.com/Class/sound/soundtoc. html

• Characteristics of Sound • Intensity of Sound: Decibels • The Ear and Its Response; Loudness • Sources of Sound: Vibrating Strings and Air Columns • Quality of Sound, and Noise; Superposition • Interference of Sound Waves; Beats • Doppler Effect • Shock Waves and the Sonic Boom

Characteristics of Sound

Sound can travel through any kind of matter, but not through a vacuum.

The speed of sound is different in different materials; in general, it is slowest in gases, faster in liquids, and fastest in solids. The speed depends somewhat on temperature, especially for gases. The speed of sound in air at and 1 atm, is 331 m/s. The speed increases approximately 0.60 m/s for each Celsius degree increase in temperature. Unless stated otherwise, assume that the temperature will be:

Loudness: related to intensity of the sound wave Pitch: related to frequency. Audible range: about 20 Hz to 20,000 Hz; upper limit decreases with age Ultrasound: above 20,000 Hz; Infrasound: below 20 Hz There are three aspects of any sound:

1. There must be a source for a sound; and as with any wave, the source of a sound must be a vibrating object.

2. The energy is transferred from the source in the form of longitudinal sound waves 3. The sound is detected by an ear or an instrument

0oC

(331 0.60 ) /v T m s

20 , so [331 (0.60)(20 )] 343 /o oC v C m s

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Sound waves are longitudinal waves traveling through a medium. The tuning fork, a common device for producing pure notes consists of two metal prongs, or tines, that vibrate when struck.

Their vibrations disturb the air near them. When a tine swings to the right the molecules in front of its movement are forced together creating a region of high molecular density called a compression (condensations).

This compression moves away from the fork like a ripple on a pond. When the tine moves to the left the molecules in the air spread apart, and the density is lower, called rarefaction (rarefactions). Example 1: Auto focusing cameras emit a pulse of very high frequency (ultrasonic) sound that travels to the object being photographed, and include a sensor that detects the returning reflected sound.

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Calculate the travel time of the pulse for an object 1.0 m away. Assume the speed of sound at 343 m/s, and the distance is to the subject and back so, 1 m + 1 m = 2 m.

Intensity of Sound: Decibels

The intensity of a wave is the energy transported per unit time across a unit area.

The human ear can detect sounds with intensity as low as 10-12

W/m2 and as high as 1 W/m2. Perceived loudness, however, is not proportional to the intensity. The loudness of a sound is much more closely related to the logarithm of the intensity. Sound level is measured in decibels (dB) and is defined:

I0 is taken to be the threshold of hearing:

An increase in sound level of 3 dB, which is a doubling in intensity, is a very small change in loudness. In open areas, the intensity of sound diminishes with distance: However, in enclosed spaces this is complicated by reflections, and if sound travels through air the higher frequencies get preferentially absorbed.

The Ear and its Response; Loudness The ear’s sensitivity varies with frequency. These curves translate the intensity into sound level at different frequencies.

2.0/ 0.0058 5.8

343 /

d mv d t t s ms

v m s

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Sources of Sound: Vibrating Strings and Air Columns Musical instruments produce sounds in various ways – vibrating strings, vibrating membranes, vibrating metal or wood shapes, vibrating air columns. The vibration may be started by plucking, striking, bowing, or blowing. The vibrations are transmitted to the air and then to our ears.

The strings on a guitar can be effectively shortened by fingering, raising the fundamental pitch. The pitch of a string of a given length can also be altered by using a string of different density.

A piano uses both methods to cover its more than seven-octave range – the lower strings (at bottom) are both much longer and much thicker than the higher ones.

Example 2: A 0.32-m-long violin string is tuned to play A above middle C at 440 Hz. a) What is the wavelength of the fundamental string vibration?

This is the wavelength of the standing wave on the string.

b) What is the wavelength of the sound wave produced? The sound wave that travels outward in the air (to reach our ears) has the same frequency, 440

Hz. The wavelength is:

Sources of Sound: Vibrating Strings and Air Columns Wind instruments create sound through standing waves in a column of air.

2 2(0.32 ) 0.64 64L m m cm

343 /0.78 78

440

v m scm

f Hz

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A tube open at both ends (most wind instruments) has pressure nodes, and therefore displacement antinodes, at the ends.

A tube closed at one end (some organ pipes) has a displacement node (and pressure antinode) at the closed end.

Example 3: What will be the fundamental frequency and first three overtones for a 26-cm-long organ pipe at room temperature if it is a) open?

b) closed?

Example 4: A flute is designed to play middle C (262 Hz) as the fundamental frequency when all the holes are covered. Approximately how long should the distance be from the mouthpiece to the far end of the flute? Assume room temp.

1

343 /660 1320 1980 2640

2 2(0.26 )

v m sf Hz Hz Hz Hz

L m

1

343 /330 990 1650 2310

4 4(0.26 )

v m sf Hz Hz Hz Hz

L m

1

343 /0.655

2 2(262 )

v m sL m

f s

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Quality of Sound, and Noise; Superposition So why does a trumpet sound different from a flute? The answer lies in overtones – which ones are present, and how strong they are, makes a big difference. The plot below shows frequency spectra for a clarinet, a piano, and a violin. The differences in overtone strength are apparent.

Interference of Sound Waves; Beats

Sound waves interfere in the same way that other waves do in space. A person at a point such as C, which is the same distance from each speaker, will experience a loud sound – the interference is constructive. At point D little if any sound – destructive.

Example 5: Two loudspeakers are 1.00 m apart. A person stands 4.00 m from one speaker. How far must this person be from the second speaker to detect destructive interference when the speakers emit an 1150-Hz sound?

For destructive interference a person must be one-half wavelength farther from one speaker than

the other, or 0.15m. Thus the person must be 3.85m or 4.15m from 2nd

speaker.

Waves can also interfere in time, causing a phenomenon called beats. Beats are the slow “envelope” around two waves that are relatively close in frequency.

343 /0.30

1150

v m sm

f Hz

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Example 6: A tuning fork produces a steady 400 Hz tone. When this tuning fork is struck and held near a vibrating guitar string, twenty beats are counted in five seconds. What are the possible frequencies produced by the guitar string?

This is the difference of the frequencies of the two waves. Because one wave is 400 Hz the other must be 404 Hz or 396 Hz.

Doppler Effect

The Doppler Effect occurs when a source of sound is moving with respect to an observer & visa versa.

At rest both observers hear same frequency. Moving left observer hears lower, right observer hears higher

If we can figure out what the change in the wavelength is, we also know the change in the frequency.

20 /5 4beatf vibrations s Hz

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The change in the wavelength is given by:

Source is moving toward the observer.

And the change in the frequency:

If the source is moving away from the observer:

If the observer is moving with respect to the source, things are a bit different. The wavelength remains the same, but the wave speed is different for the observer.

We find, for an observer moving towards a stationary source:

And if it is moving away:

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Example 7: The siren of a police car at rest emits at a frequency of 1600 Hz. What frequency will you hear if you are at rest and the police car moves at 25.0 m/s a) towards you?

b) away from you?

Example 8: A 5000 Hz sound wave is emitted by a stationary source. This sound wave reflects from an object moving 3.50 m/s toward the source. What is the frequency of the wave reflected by the moving object as detected by a detector at rest near the source?

The frequency f ’ that is detected by the moving object is:

The moving object now emits (reflects) a sound of frequency:

Thus the frequency shifts by 103 Hz.

Shock Waves and the Sonic Boom

If a source is moving faster than the wave speed in a medium, waves cannot keep up and a shock wave is formed. The angle of the cone is:

1600' 1726

25.0 /11

343 /source

sound

f Hzf Hz

m sv

m sv

1600' 1491

25.0 /11

343 /source

sound

f Hzf Hz

m sv

m sv

3.50 /' 1 1 (5000 ) 5051

343 /

obs

snd

v m sf f Hz Hz

vs m s

' 5051" 5103

3.50 /11

343 /source

nd

f Hzf Hz

m sv

m sv

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Shock waves are analogous to the bow waves produced by a boat going faster than the wave speed in water.

Aircraft exceeding the speed of sound in air will produce two sonic booms, one from the front and one from the tail.

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CHAPTER 11/12

WAVES AND VIBRATIONS

CONCEPTS

1. A characteristic common to sound waves and light waves is that they transfer

energy.

2. Light is to brightness as sound is to loudness.

3. A beam of light entering a glass prism obliquely (at an angle) and

emerging as a band of colors illustrates the process of dispersion.

4. The diagram to the right shows white light being dispersed as it

passes from air into a glass prism. This phenomenon occurs because

in glass each frequency of light has a different absolute index of

refraction.

5. A laser beam does not disperse as it passes through a prism because the

laser beam is monochromatic.

6. The diagram to the right represents waves passing through a small

opening in a barrier. This is an example of diffraction.

7. Diffraction and interference will occur when light passes through a

double slit.

8. All electromagnetic waves have the same speed in a vacuum.

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9. The pattern of light produced by the interaction of light with a

thin film is the result of interference.

10. The color spectrum ranges in order from: red, orange, yellow,

green, blue, indigo, and violet.

11. In a nondispersive medium, the speed of light waves depends on the nature of the medium.

12. As the energy imparted to a mechanical wave increases, the maximum displacement

of the particles in the medium increases.

13. A single vibratory disturbance which moves from point to point in a material

is known as a pulse.

14. As a pulse travels through a stretched heavy rope attached to a light

rope its speed will increase as it travels through the light rope.

15. The diagram to the right shows a transverse water wave moving in the

direction shown by the velocity vector v. At the instant shown, a cork

at point P on the water’s surface is moving toward B.

16. Whether or not a wave is longitudinal or transverse may be determined by

its ability to be polarized.

17. As a wave is refracted, the frequency of the wave will remain unchanged.

18. The graph that best represents the relationship between the frequency and

period of a wave is C.

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19. The change in direction of a wave when it passes obliquely from one

medium to another is called refraction.

20. As observed from the Earth, the light from a star is shifted toward lower frequencies. This is an

indication that the distance between the Earth and the star is increasing.

21. As the period of a wave decreases, the wave’s frequency increases.

22. Two waves have the same frequency. They must also have identical periods.

23. In the diagram to the right, the distance between points A and B on a

wave is 0.10 m. This wave must have a wavelength of 0.20 m.

24. As a wave enters a medium, there may be a change in the wave’s speed.

25. Only coherent wave sources produce waves that have a constant phase relation.

26. A sound wave can not be polarized.

27. If the frequency of a sound wave in air at STP remains constant, its energy can be varied by

changing its amplitude.

28. An observer detects an apparent change in the frequency of sound

Waves produced by an airplane passing overhead. This phenomenon

illustrates the Doppler effect.

29. The vibrating tuning fork shown to the right produces a constant frequency.

The tuning fork is moving to the right at a constant speed, and observers

are located at points A, B, C, and D. The observer at D hears the lowest

frequency.

30. Interference occurs when two or more waves pass simultaneously through the same region

in a medium.

31. An opera singer’s voice is able to break a thin crystal glass if the singer’s voice

and the glass have the same natural frequency.

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32. Standing waves are produced by the interference of two waves with the same frequency and

amplitude but opposite directions.

33. When the stretched string of the apparatus on the right is made to

vibrate, point P does not move. Point P is most probably at the location

of a node.

34. The distance between successive antinodes in the standing wave pattern

shown to the right is equal to ½ wavelength.

35. Maximum destructive interference between two waves occurs when the waves are out of phase

by 180 degrees.

36. The diagram on the right represents a group of light waves emitted

simultaneously from a single light source. The light waves would be

classified as both monochromatic and coherent.

37. Refraction of a wave is caused by a change in the wave’s speed.

38. As a periodic wave travels from one medium to another, the period and frequency of that wave

cannot change.