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Chapter 16
Waves and Sound
16.1 The Nature of Waves
1. A wave is a traveling disturbance.
2. A wave carries energy from place to place.
16.1 The Nature of Waves
Transverse Wave
16.1 The Nature of Waves
Longitudinal Wave
16.1 The Nature of Waves
Water waves are partially transverse and partially longitudinal.
16.2 Periodic Waves
Periodic waves consist of cycles or patterns that are produced over and
over again by the source.
In the figures, every segment of the slinky vibrates in simple harmonic
motion
16.2 Periodic Waves
In the drawing, one cycle is shaded in color.
The amplitude A is the maximum excursion of a particle of the medium from
the particles undisturbed position.
The wavelength is the horizontal length of one cycle of the wave.
The period is the time required for one complete cycle.
The frequency is related to the period and has units of Hz, or s-1
.
T
f
1
=
16.2 Periodic Waves
λ
λ
f
T
v ==
16.2 Periodic Waves
Example 1 The Wavelengths of Radio Waves
AM and FM radio waves are transverse waves consisting of electric and
magnetic field disturbances traveling at a speed of 3.00x108
m/s. A station
broadcasts AM radio waves whose frequency is 1230x103
Hz and an FM
radio wave whose frequency is 91.9x106
Hz. Find the distance between
adjacent crests in each wave.
λ
λ
f
T
v ==
f
v
=λ
16.2 Periodic Waves
AM m244
Hz101230
sm1000.3
3
8
=
×
×
==
f
v
λ
FM m26.3
Hz1091.9
sm1000.3
6
8
=
×
×
==
f
v
λ
16.3 The Speed of a Wave on a String
The speed at which the wave moves to the right depends on how quickly
one particle of the string is accelerated upward in response to the net
pulling force.
Lm
F
v =
tension
Length of string
16.3 The Speed of a Wave on a String
Example 2 Waves Traveling on Guitar Strings
Transverse waves travel on each string of an electric guitar after the
string is plucked. The length of each string between its two fixed ends
is 0.628 m, and the mass is 0.208 g for the highest pitched E string and
3.32 g for the lowest pitched E string. Each string is under a tension
of 226 N. Find the speeds of the waves on the two strings.
16.3 The Speed of a Wave on a String
High E
( ) ( )
sm826
m0.628kg100.208
N226
3-
=
×
==
Lm
F
v
Low E
( ) ( )
sm207
m0.628kg103.32
N226
3-
=
×
==
Lm
F
v
16.5 The Nature of Sound Waves
LONGITUDINAL SOUND WAVES
The area of condensation is
the region of compression
with increased air pressure
The area of rarefaction is
the region behind the
condensation with
decreased air pressure
16.5 The Nature of Sound Waves
Individual air molecules are not carried along with the wave.
16.5 The Nature of Sound Waves
THE FREQUENCY OF A SOUND WAVE
The frequency is the number of cycles
per second.
A sound with a single frequency is called
a pure tone.
The brain interprets the frequency in terms
of the subjective quality called pitch.
16.5 The Nature of Sound Waves
THE PRESSURE AMPLITUDE OF A SOUND WAVE
Loudness is an attribute of
a sound that depends primarily
on the pressure amplitude
of the wave.
Larger amplitude = Louder sound
16.6 The Speed of Sound
Sound travels through gases,
liquids, and solids at considerably
different speeds.
16.6 The Speed of Sound
Conceptual Example 5 Lightning, Thunder, and a Rule of Thumb
There is a rule of thumb for estimating how far away a thunderstorm is.
After you see a flash of lighting, count off the seconds until the thunder
is heard. Divide the number of seconds by five. The result gives the
approximate distance (in miles) to the thunderstorm. Why does this
rule work?
16.6 The Speed of Sound
LIQUIDS SOLID BARS
ρ
adB
v =
ρ
Y
v =
Page 304
Page 322
Page 308
16.8 Decibels
The decibel (dB) is a measurement unit used when comparing two sound
intensities.
Because of the way in which the human hearing mechanism responds to
intensity, it is appropriate to use a logarithmic scale called the intensity
level:
( ) 





=
oI
I
logdB10β
212
mW1000.1 −
×=oI
Note that log(1)=0, so when the intensity
of the sound is equal to the threshold of
hearing, the intensity level is zero.
16.8 Decibels
( ) 





=
oI
I
logdB10β
212
mW1000.1 −
×=oI
16.9 The Doppler Effect
The Doppler effect is the
change in frequency or pitch
of the sound detected by
an observer because the sound
source and the observer have
different velocities with respect
to the medium of sound
propagation.
16.10 Applications of Sound in Medicine
By scanning ultrasonic waves across the body and detecting the echoes
from various locations, it is possible to obtain an image.
16.10 Applications of Sound in Medicine
Ultrasonic sound waves cause
the tip of the probe to vibrate at
23 kHz and shatter sections of
the tumor that it touches.

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Chapter16powerpoint 090408180549-phpapp01

  • 2. 16.1 The Nature of Waves 1. A wave is a traveling disturbance. 2. A wave carries energy from place to place.
  • 3. 16.1 The Nature of Waves Transverse Wave
  • 4. 16.1 The Nature of Waves Longitudinal Wave
  • 5. 16.1 The Nature of Waves Water waves are partially transverse and partially longitudinal.
  • 6. 16.2 Periodic Waves Periodic waves consist of cycles or patterns that are produced over and over again by the source. In the figures, every segment of the slinky vibrates in simple harmonic motion
  • 7. 16.2 Periodic Waves In the drawing, one cycle is shaded in color. The amplitude A is the maximum excursion of a particle of the medium from the particles undisturbed position. The wavelength is the horizontal length of one cycle of the wave. The period is the time required for one complete cycle. The frequency is related to the period and has units of Hz, or s-1 . T f 1 =
  • 9. 16.2 Periodic Waves Example 1 The Wavelengths of Radio Waves AM and FM radio waves are transverse waves consisting of electric and magnetic field disturbances traveling at a speed of 3.00x108 m/s. A station broadcasts AM radio waves whose frequency is 1230x103 Hz and an FM radio wave whose frequency is 91.9x106 Hz. Find the distance between adjacent crests in each wave. λ λ f T v == f v =λ
  • 10. 16.2 Periodic Waves AM m244 Hz101230 sm1000.3 3 8 = × × == f v λ FM m26.3 Hz1091.9 sm1000.3 6 8 = × × == f v λ
  • 11. 16.3 The Speed of a Wave on a String The speed at which the wave moves to the right depends on how quickly one particle of the string is accelerated upward in response to the net pulling force. Lm F v = tension Length of string
  • 12. 16.3 The Speed of a Wave on a String Example 2 Waves Traveling on Guitar Strings Transverse waves travel on each string of an electric guitar after the string is plucked. The length of each string between its two fixed ends is 0.628 m, and the mass is 0.208 g for the highest pitched E string and 3.32 g for the lowest pitched E string. Each string is under a tension of 226 N. Find the speeds of the waves on the two strings.
  • 13. 16.3 The Speed of a Wave on a String High E ( ) ( ) sm826 m0.628kg100.208 N226 3- = × == Lm F v Low E ( ) ( ) sm207 m0.628kg103.32 N226 3- = × == Lm F v
  • 14. 16.5 The Nature of Sound Waves LONGITUDINAL SOUND WAVES The area of condensation is the region of compression with increased air pressure The area of rarefaction is the region behind the condensation with decreased air pressure
  • 15. 16.5 The Nature of Sound Waves Individual air molecules are not carried along with the wave.
  • 16. 16.5 The Nature of Sound Waves THE FREQUENCY OF A SOUND WAVE The frequency is the number of cycles per second. A sound with a single frequency is called a pure tone. The brain interprets the frequency in terms of the subjective quality called pitch.
  • 17. 16.5 The Nature of Sound Waves THE PRESSURE AMPLITUDE OF A SOUND WAVE Loudness is an attribute of a sound that depends primarily on the pressure amplitude of the wave. Larger amplitude = Louder sound
  • 18. 16.6 The Speed of Sound Sound travels through gases, liquids, and solids at considerably different speeds.
  • 19. 16.6 The Speed of Sound Conceptual Example 5 Lightning, Thunder, and a Rule of Thumb There is a rule of thumb for estimating how far away a thunderstorm is. After you see a flash of lighting, count off the seconds until the thunder is heard. Divide the number of seconds by five. The result gives the approximate distance (in miles) to the thunderstorm. Why does this rule work?
  • 20. 16.6 The Speed of Sound LIQUIDS SOLID BARS ρ adB v = ρ Y v = Page 304 Page 322 Page 308
  • 21. 16.8 Decibels The decibel (dB) is a measurement unit used when comparing two sound intensities. Because of the way in which the human hearing mechanism responds to intensity, it is appropriate to use a logarithmic scale called the intensity level: ( )       = oI I logdB10β 212 mW1000.1 − ×=oI Note that log(1)=0, so when the intensity of the sound is equal to the threshold of hearing, the intensity level is zero.
  • 22. 16.8 Decibels ( )       = oI I logdB10β 212 mW1000.1 − ×=oI
  • 23. 16.9 The Doppler Effect The Doppler effect is the change in frequency or pitch of the sound detected by an observer because the sound source and the observer have different velocities with respect to the medium of sound propagation.
  • 24. 16.10 Applications of Sound in Medicine By scanning ultrasonic waves across the body and detecting the echoes from various locations, it is possible to obtain an image.
  • 25. 16.10 Applications of Sound in Medicine Ultrasonic sound waves cause the tip of the probe to vibrate at 23 kHz and shatter sections of the tumor that it touches.