phy238y lecture 8 sound waves the speed of sound traveling sound waves intensity and sound level...
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PHY238YLecture 8
Sound waves The speed of sound Traveling sound waves Intensity and sound level
References: Haliday, Resnick, Walker: Fundamentals of Physics, 6th ed., Wiley 2003, Ch. 18 (18.1 – 18.3, 18.5)
Hallett et al.: Physics for the life sciences, 4th ed., Ch.2 (2.1 – 2.5)Thanks to dr. R. Nave for the permission to use some of the pictures from Hyper
Physics: http://hyperphysics.phy-astr.gsu.edu
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PHY238YLecture 8
Sound waves are longitudinal
A single-frequency sound wave traveling through air will cause a sinusoidal pressure variation in the air.
The air motion which accompanies the passage of the sound wave will be back and forth in the direction of the propagation of the sound. tkxss m cos
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PHY238YLecture 8
The elastic property of a gas or liquid is called bulk modulus
The speed of sound:
density
bulkBwhere
B
propertyinertial
propertyelasticv
modulus
:
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PHY238YLecture 8
Sound pressure: Audible sound consists of pressure waves Sound pressure pm is defined as the amplitude of the pressure wave The power carried by the wave is proportional to the square of the amplitude
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PHY238YLecture 8
Traveling sound waves: Displacement and
pressure variations
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PHY238YLecture 8
Sound intensity is
Power/unit area
or: time rate of energy transfer/unit area Many sound intensity measurements are made relative to a standard
threshold of hearing intensity I0, The most common approach to sound intensity measurement is to
measure the sound level on the decibel scale:
2162120 /10/10 cmWattsmWattsI
010log10)(I
IdBI
The factor of 10 multiplying the logarithm makes it decibels instead of Bels, and is included because ~ 1 decibel is the just noticeable difference (JND) in sound intensity for the normal human ear
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PHY238YLecture 8
The threshold of hearing
The measured threshold of hearing curve shows that the sound intensity required to be heard is quite different for different frequencies.
The standard threshold of hearing at 1000 Hz is nominally taken to be 0 dB (it actually is 4 dB)
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PHY238YLecture 8
Threshold of pain is 120 – 130 dB
The dynamic range of human hearing extends from zero dB to the threshold of pain.
Example: problem 18-2 p. 404 from Halliday/Resnick/Walker
Intensity level (dB)
Ear drum rupture 160
Pain threshold 120-130
Shotgun blast 100
Car horn (6 m distance)
90
City street 75
Typical room 40
Open country 10
Threshold of hearing
0
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PHY238YLecture 8
The audible sound: a pressure wave with frequency between 20 Hz and 20,000 Hz and with an intensity above the standard threshold of hearing:
Frequency: 20 Hz - 20,000 Hz (corresponds with pitch) Wavelength (at 20oC in air): 0.0172m – 17.2 m Intensity: 10-12 - 10 W/m2 (0 to 130 dB) Pressure: 2 x 10-5 - 60 N/m2 (2 x 10-10 - .0006 atm) Sounds may be generally characterized by:
Pitch (frequency) Loudness (is NOT simply the intensity level) Quality (timbre – determined by the harmonic content of the
sound)
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PHY238YLecture 8
Variation of intensity with distance: the inverse square law:
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PHY238YLecture 8
Inverse square law plot