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Physics of Sound

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Speech frequencies: generally regarded to be 500 to 3000 hertz. Frequency range of perceivable sound: 20 Hz to 15,000 to 20,000 Hertz. Tuning forks ... – PowerPoint PPT presentation

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Title: Physics of Sound


1
Physics of Sound
2
Logarithms
  • Do you know how to use your calculator?
  • Find the following functions
  • , - , x , / , , log
  • The log is the exponent to which 10 is raised,
    representing a number

3
Antilogarithm
  • The antilog is 10 raised to the x power, or 10x

4
Logarithms
  • Solve the following together
  • Log (20) ___________
  • Log (400) ____________
  • Solve on your own
  • Log (0.5) ____________
  • Log 2 _____________

5
Antilogarithms
  • Solve the following together
  • X 2 _______________
  • X 4.3 _______________
  • Solve on your own
  • X 8.5 _____________
  • X 9.0 _____________

6
What is sound?
  • Any change in air pressure
  • The molecules in the air exerts a pressure of
    over 1 ton per square foot on our ears
  • Must be a rapid change in sound pressure to be
    heard, a small rapid change will create noise
  • Travels as sound waves

7
Frequency of Sound
  • Rate at which complete high and low pressure
    regions are produced by the sound source.
  • 1000 cycles per second is 1000 high and low
    pressure regions passing a point in one second.
    This is called 1000 Hertz (Hz) or 1 kHz.

8
Speech frequencies
  • Speech frequencies generally regarded to be 500
    to 3000 hertz
  • Frequency range of perceivable sound 20 Hz to
    15,000 to 20,000 Hertz.
  • Tuning forks

9
Tone and Noise
  • Tuning fork pure tone and related frequencies
  • We cannot see the tines moving back and forth
    because they are moving back and for the too
    quickly. Two-hundred cycles a second is too fast
    to see.
  • Noise random frequencies

10
Noise travels through a medium
  • A vibrating object creates a disturbance that
    travels through a medium
  • A trains noise can travel through the steel
    tracks by creating sound waves
  • The vibrations of a speaker creates sound waves
  • Frequency is the number of complete back and
    forth vibrations per second

11
Noise travel
  • Vibrational motion of the medium is set up by the
    object.
  • The vibrations set the molecule of the medium
    into motion.
  • The motion of the molecule in the medium sets the
    molecule next to it, in motion.
  • The transfer of energy continues as the vibration
    of one molecule sets the next molecule into
    motion.

12
Sound wave is a pressure wave
  • Thus an instrument can be used to measure the
    oscillations of high and low pressure variations
    in the pressure.
  • These oscillations are shown as the typical sine
    wave that you may have seen

13
Wavelength
  • Distance which a disturbance travels along the
    medium in one complete wave cycle.
  • Measured from one wave trough or crest to the
    next wave trough or crest, in a transverse wave.
    It is from one wave compression to the next wave
    compression in a longitudinal wave
  • With a pressure wave it is from one high pressure
    region to the next high pressure region

14
Speed of Sound
  • Sound waves are pressure disturbances traveling
    through a medium by means of particle interaction
  • How fast the disturbance is passed from particle
    to particle determines the speed of sound.
  • How easily the medium transfers the disturbance
    determines the speed, which is measured in feet
    per second (ft/sec)

15
Speed of Sound
  • Speed is equal to distance traveled per unit
    time.
  • Speed distance/time
  • If a sound waves travels 2,300 feet in 2 seconds
    the sound is traveling at 1,150 ft/sec
  • Examples of sound travel would be the time it
    takes for thunder to reach the observer and an
    echo

16
Speed of Sound
  • The speed depends on the properties of the
    medium, the elastic properties are much greater
    than are the inertial properties.
  • Thus longitudinal sound waves will travel faster
    in solids than in liquids, and longitudinal sound
    waves will travel faster in liquids than in gases

17
Speed of Sound in air
  • The speed of sound in air will depend on
    temperature and pressure of the air. The
    relationship is
  • C 1054 f/s (1.07 f/s/oF)xT

18
Speed of Sound
  • At 72 oF, the speed of sound is 1,130 f/s
  • The delay between lightning and thunder.
  • Light travels 980,000,000 f/s or reaches the
    observer in almost no time.
  • The time delay of an echo is the same phenomenon,
    the distance of a reflecting surface can be
    determined by the time it takes for the echo to
    return

19
Speed of Sound
  • The speed of sound in different mediums at
    standard conditions
  • In air the velocity is 1,130 f/s
  • In water the velocity is 4,700 f/s
  • In wood the velocity is 13,000 f/s
  • In steel the velocity is 16,500 f/s

20
Speed, frequency and wavelength
  • The mathematical relationship between the three
    is
  • C ? x f
  • The speed is a constant based on the properties
    of the medium. The length of a wave will vary
    with the frequency.

21
Speed, frequency and wavelength
  • At standard conditions, the speed of sound is
    1,130 f/s. Say we have a 440 hertz frequency
    pure tone sound, what is the wavelength of the
    sound?
  • C ? x f
  • ? C / f
  • ? 1,130 / 440
  • ? 2.57 feet

22
Speed, frequency and wavelength
  • How about air at 1,000 oF as part of an exhaust
    stream?
  • Find the speed of sound traveling through the
    exhaust?
  • C 1,054 f/s (1.07 f/s)x oF
  • C 1,054 1.071,000
  • C 1,054 1070 2,124 f/s

23
Speed, frequency and wavelength
  • Engine rotating at 3,000 rpm and has 4 cylinders
  • 3,000 4 12,000 rounds per minute
  • Which equals 200 rounds per second (Hz)
  • What is the frequency of this sound?
  • ? C / f
  • ? 2,124 / 200
  • ? 10.62 ft

24
Speed, frequency and wavelength
  • What is the wavelength of the following
    frequencies? (at standard conditions)
  • ? 20 hz ________ remember ? C/f
  • ? 1000 hz ________
  • ? 16000 hz ________

25
Period
  • The period is the time for one complete cycle of
    pressure transition. It is the reciprocal of the
    frequency.
  • T (sec) 1/f
  • The period of a 1000 Hz sound wave is
  • T 1/f 1/1000 0.001 seconds

26
Period
  • What is the period of a 20 Hz and a 16,000 Hz
    wave?
  • T20 Hz 1/f
  • T16000 Hz 1/f

27
Period
  • Below 20 Hz infrasound
  • Above 20,000 Hz ultrasound
  • Dogs 50 Hz to 45,000 Hz
  • Cats 45 Hz to 85,000 Hz
  • Bats to 120,000 Hz
  • Dolphins 200,000 Hz
  • Elephant down to 5 Hz and up to 10,000 Hz

28
Sound Waves
  • A pure tone (tuning fork) sound introduced into
    the room will create a change in the molecules in
    the room.
  • At 440 Hz the molecules will bunch up every 3
    feet
  • Also there will be a net drift of molecules from
    the bunched up section to the section where the
    molecules are further apart.
  • The wave is moving toward me at 1,130 f/s

29
Sound Waves
  • The sound wave is traveling toward me however,
    the molecules are not moving toward me.
  • An example would be a garden hose, when I shake
    it a snaky wave travels away, however, the hose
    is not moving only the wave energy is moving
    along it.
  • Other examples would include sound, water, and
    football fans

30
Sound Waves
  • Mechanical waves they require a medium to
    transfer energy. So sound will not transfer
    through a vacuum.
  • Slinky demo
  • Pulse and a wave moves one coil at a time
  • Medium is the slinky. In water it is the water,
    at a concert it is the air, at a football game
    its the fans in the stadium

31
Intensity
  • The amount of energy which is transported past a
    given area of the medium per unit time
  • Intensity energy / (time x area)
  • Since power is energy per unit time, it can also
    be written as
  • Intensity power / area
  • Typical units are Watts/meter2

32
Intensity
  • Inverse square relationship
  • The mathematical relationship of intensity and
    the distance from the source
  • As you move away from the source (larger
    distance) the area gets larger and the intensity
    will decrease.
  • If the distance from a source doubles the
    intensity will decrease by a factor of 4.

33
Threshold of Hearing
  • Humans can detect sound of very low intensity.
    The faintest sound which the ear can detect has
    an intensity of 1x10-12 W/m2.
  • At this level sound will displace particles of
    air by a mere one-billionth of a centimeter.

34
Loudness
  • Loudness of a noise is a more subjective
    response. Factors that affect the perception of
    loudness includes age and frequency

35
Sound Intensity
  • The average rate at which sound energy is flowing
    through a unit area
  • Intensity can be measured by means of a twin
    microphone probe, with signal processing by a
    microprocessor controlled cross correlation
    spectrum analyzer
  • Measurement of intensity is very useful in
    industrial noise situations

36
Decibels
  • The decibel scale is a logarithmic scale. The
    logarithmic scale is based on multiples of 10.
  • A sound which is 10 times more intense is
    assigned a sound level of 10 dB.
  • A sound which is 100 times more intense is
    assigned a sound level of 20 dB.
  • A sound which is 1000 times more intense is
    assigned a sound level of 30 dB.

37
Decibels
  • Threshold of hearing 0 dB
  • Whisper 20 dB
  • Normal conversation 60 dB
  • Street traffic 70 dB
  • Vacuum cleaner 80 dB
  • Walkman at max setting 100 dB
  • Threshold of Pain 130 dB
  • Military Jet Takeoff 140 dB

38
Sound Pressure and Sound Pressure Level
  • Sound pressure is the root mean square (rms)
    value of the pressure changes above and below
    atmospheric when used to measure steady state
    noise.
  • The sound pressure level is the ratio expressed
    in decibels (dB) of the rms pressure to a
    reference rms pressure.

39
Sound Pressure Level
  • Sound pressure level (Lp) is
  • Lp 10 log (P / Po)2
  • 20 log (P / Po)
  • Where Po the reference sound pressure of 2 x
    10-5 N/m2
  • Lp sound pressure level in dB
  • P rms sound pressure in N/m2

40
Sound Pressure Level
  • For a sound source having a sound pressure of 1
    N/m2, what is the sound pressure level in dB?
  • Lp 20 log (P/Po)
  • 20 log ((1 N/m2)/(2x10-5 N/m2)
  • 20 log (0.5 x 105) 94 dB

41
Sound Pressure Level
  • If the sound source has a sound pressure of
    2x10-3 N/m2, what is the sound pressure level in
    dB?

42
Sound Pressure Level
  • If the sound source has a sound pressure of
    2x10-3 N/m2, what is the sound pressure level in
    dB?
  • Lp 20 log (P/Po)
  • 20 log ((2x10-3 N/m2)/(2x10-5 N/m2)
  • 20 log (1 x 102) 40 dB

43
Sound Pressure Level
  • Weighted sound levels Fletcher-Munson curves.
  • Ear is most sensitive around 2 to 5 kHz

44
Decibel Addition
  • To add individual sound levels the equation to
    add these is
  • LT 10log(10L1/1010L2/1010L3/10 10Ln/10)
  • Example Two machines each operate at 93 dB at a
    given location. What is the sound pressure level
    if both machines are on?

45
Decibel Addition
  • Add to sound pressure levels of 93 dB together
  • LT 10log(10L1/10 10L2/10)
  • LT 10log(1093/10 1093/10)
  • LT 10log(2 x 109.3) 96 dB

46
Decibel Addition
  • Exercise Three machines have the following
    sound pressure levels at a given measurement
    location 95, 96, 100 dB
  • What is the resulting sound pressure level if all
    three machines are on?

47
Decibel Addition
  • Rule of thumb (can only be used when a limited
    number of sources are added together)
  • 0 dB difference add 3 dB to the higher value
  • 1-1.5 dB difference add 2.5 dB
  • 2-3 dB difference add 2 dB
  • 3.5 to 4.5 dB add 1.5 dB
  • 5 to 7 dB add 1 dB
  • 7.5 to 13 dB add 0.5 dB

48
Decibel Addition
  • Using the rule of thumb in the previous exercise,
    find the total sound pressure level

49
Sound Pressure Level in decibels of common
sources of noise
  • See page 38 and 39 in your manual
  • Examples refrigerator 50 dB
  • rainfall 50 dB
  • doorbell 80 dB
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