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Sound

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Title: Sound


1
Chapter 12
  • Sound

2
Sound, A special kind of longitudinal wave
Consider a vibrating guitar string
3
Sound
  • Producing a Sound Wave
  • Sound waves are longitudinal waves traveling
    through a medium
  • A tuning fork can be used as an example of
    producing a sound wave

4
Using a Tuning Fork to Produce a Sound Wave
  • A tuning fork will produce a pure musical note
  • As the tines vibrate, they disturb the air near
    them
  • As the tine swings to the right, it forces the
    air molecules near it closer together
  • This produces a high density area in the air
  • This is an area of compression

5
Using a Tuning Fork, cont.
  • As the tine moves toward the left, the air
    molecules to the right of the tine spread out
  • This produces an area of low density
  • This area is called a rarefaction

6
Using a Tuning Fork, final
  • As the tuning fork continues to vibrate, a
    succession of compressions and rarefactions
    spread out from the fork
  • A sinusoidal curve can be used to represent the
    longitudinal wave
  • Crests correspond to compressions and troughs to
    rarefactions

7
What IS Sound?
  • Sound is really tiny fluctuations of air pressure
  • units of pressure N/m2 or psi (lbs/square-inch)
  • Carried through air at 343 m/s (770 m.p.h) as
    compressions and rarefactions in air pressure

wavelength
compressed gas
rarefied gas
8
Properties of Waves
? or T
pressure
horizontal axis could be space representing
snapshot in time time representing sequence at
a par- ticular point in space
  • Wavelength (?) is measured from crest-to-crest
  • or trough-to-trough, or upswing to upswing, etc.
  • For traveling waves (sound, light, water), there
    is a speed (c)
  • Frequency (f) refers to how many cycles pass by
    per second
  • measured in Hertz, or Hz cycles per second
  • associated with this is period T 1/f
  • These three are closely related
  • ?f v

9
Characteristics of Sound Waves
  • Pitch refers to whether the sound is a high or
    low note (pitch -gt frequency)
  • Audible waves
  • Lay within the normal range of hearing of the
    human ear
  • Normally between 20 Hz to 20,000 Hz
  • Infrasonic waves
  • Frequencies are below the audible range
  • Earthquakes are an example
  • Ultrasonic waves
  • Frequencies are above the audible range
  • Dog whistles are an example

10
Longitudinal vs. Transverse Waves
  • Sound is a longitudinal wave, meaning that the
    motion of particles is along the direction of
    propagation
  • Transverse waveswater waves, lighthave things
    moving perpendicular to the direction of
    propagation

11
Why is Sound Longitudinal?
  • Waves in air cant really be transverse, because
    the atoms/molecules are not bound to each other
  • cant pull a (momentarily) neighboring molecule
    sideways
  • only if a rubber band connected the molecules
    would this work
  • fancy way of saying this gases cant support
    shear loads
  • Air molecules can really only bump into one
    another
  • Imagine people in a crowded train station with
    hands in pockets
  • pushing into crowd would send a wave of
    compression into the crowd in the direction of
    push (longitudinal)
  • jerking people back and forth (sideways, over
    several meters) would not propagate into the
    crowd
  • but if everyone held hands (bonds), this
    transverse motion would propagate into crowd

12
Speed of Sound
  • Sound speed in air is related to the frantic
    motions of molecules as they jostle and collide
  • since air has a lot of empty space, the
    communication that a wave is coming through has
    to be carried by the motion of particles
  • for air, this motion is about 500 m/s, but only
    about 350 m/s directed in any particular
    direction
  • Solids have faster sound speeds because atoms are
    hooked up by springs (bonds)
  • dont have to rely on atoms to traverse gap
  • spring compression can (and does) travel faster
    than actual atom motion

13
Example Sound Speeds
Medium sound speed (m/s)
air (0?C) 331
air (20?C) 343
water 1497
gold 3240
brick 3650
wood 38004600
glass 5100
steel 5790
aluminum 6420
14
The Speed of Sound
  • Speed of Sound in a Liquid
  • In a liquid, the speed depends on the liquids
    compressibility and inertia
  • B is the Bulk Modulus of the liquid
  • ? is the density of the liquid
  • Compares with the equation for a transverse wave
    on a string

15
Speed of Sound in a Solid Rod
  • The speed depends on the rods compressibility
    and inertial properties
  • Y is the Youngs Modulus of the material
  • ? is the density of the material

16
Speed of Sound, General
  • The speed of sound is higher in solids than in
    gases
  • The molecules in a solid interact more strongly
  • The speed is slower in liquids than in solids
  • Liquids are more compressible

Medium Speed (m/s)
Air 343
Helium 972
Water 1500
Steel (solid) 5600
17
Speed of Sound in Air
  • 331 m/s is the speed of sound at 0 C
  • T is the absolute temperature

18
Speed of Sound
  • Mach Number Object speed/ Speed of Sound

19
Speed of Sound
  • Example
  • The speed of sound in a column of air is measured
    to be 356 m/s. What is the temperature of the air?

20
Energy and Intensity of Sound Waves
  • Intensity of Sound Waves
  • The average intensity of a wave is the rate at
    which the energy flows through a unit area, A,
    oriented perpendicular to the direction of travel
    of the wave
  • The rate of energy transfer is the power
  • Units are W/m2

21
Various Intensities of Sound
  • Threshold of hearing
  • Faintest sound most humans can hear
  • About 1 x 10-12 W/m2
  • Threshold of pain
  • Loudest sound most humans can tolerate
  • About 1 W/m2
  • The ear is a very sensitive detector of sound
    waves
  • It can detect pressure fluctuations as small as
    about 3 parts in 1010

22
Intensity Level of Sound Waves
  • The sensation of loudness is logarithmic in the
    human hear
  • ß is the intensity level or the decibel level of
    the sound
  • Io is the threshold of hearing

23
Various Intensity Levels
  • Threshold of hearing is 0 dB
  • Threshold of pain is 120 dB
  • Jet airplanes are about 150 dB
  • Table 14.2 lists intensity
  • levels of various sounds
  • Multiplying a given intensity by 10 adds 10 dB to
    the intensity level

24
Intensity of sounds
  • Some examples (1 pascal ? 10-5 atm)

Sound Intensity Pressure Intensity amplitud
e (Pa) (W/m2) level (dB) Hearing threshold 3 ?
10-5 10-12 0 Classroom 0.01 10-7
50 City street 0.3 10-4 80 Car without
muffler 3 10-2 100 Indoor concert 30 1 120 Jet
engine at 30 m. 100 10 130
25
Energy/Intensity Waves
  • Example
  • A family ice show is held at an enclosed area.
    The skaters perform to music playing at a level
    of 80.0 dB. The intensity level of music playing
    is too loud for your baby brother who yells at
    75.0 dB. (a) What total sound intensity is
    produced? (b) What is the combined sound level?

26
The Doppler Effect
  • A Doppler effect is experienced whenever there is
    relative motion between a source of waves and an
    observer.
  • When the source and the observer are moving
    toward each other, the observer hears a higher
    frequency
  • When the source and the observer are moving away
    from each other, the observer hears a lower
    frequency

27
Doppler Effect, cont.
  • Although the Doppler Effect is commonly
    experienced with sound waves, it is a phenomena
    common to all waves
  • Assumptions
  • The air is stationary
  • All speed measurements are made relative to the
    stationary medium

28
Doppler Effect, Case 1 (Observer Toward Source)
  • An observer is moving toward a stationary source
  • Due to his movement, the observer detects an
    additional number of wave fronts
  • The frequency heard is increased

29
Doppler Effect, Case 1(Observer Away from Source)
  • An observer is moving away from a stationary
    source
  • The observer detects fewer wave fronts per second
  • The frequency appears lower

30
Doppler Effect, Case 1 Equation
  • When moving toward the stationary source, the
    observed frequency is
  • When moving away from the stationary source,
    substitute vo for vo in the above equation

31
Doppler Effect, Case 2 (Source in Motion)
  • As the source moves toward the observer (A), the
    wavelength appears shorter and the frequency
    increases
  • As the source moves away from the observer (B),
    the wavelength appears longer and the frequency
    appears to be lower

32
Doppler Effect, Source Moving Equation
  • Use the vs when the source is moving toward the
    observer and vs when the source is moving away
    from the observer

33
Doppler Effect, General Case
  • Both the source and the observer could be moving
  • Use positive values of vo and vs if the motion is
    toward
  • Frequency appears higher
  • Use negative values of vo and vs if the motion is
    away
  • Frequency appears lower

34
Doppler Effect
  • Example
  • As a truck travelling at 96 km/hr approaches and
    passes a person standing along the highway, the
    driver sounds the horn. If the horn has a
    frequency of 400 Hz, what are the frequencies of
    the sound waves heard by the person
  • (a) as the truck approaches?
  • (b) after it has passed?
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