Nicholas J. Giordano
www.cengage.com/physics/giordano
Chapter 12 Waves
Wave Motion • A wave is a moving disturbance that transports
energy from one place to another without transporting matter
• Questions about waves • What is being disturbed? • How is it disturbed?
• The motion associated with a wave disturbance often has a repeating form, so wave motion has much in common with simple harmonic motion
Introduction
Waves, String Example
• One example of a wave is a disturbance on a string • Shaking the free end creates a disturbance that moves
horizontally along the string • A single shake creates a wave pulse • If the end of the string is shaken up and down in simple
harmonic motion, a periodic wave is produced Section 12.1
Waves, String Example cont. • The disturbances are examples of waves • Portions of the string are moving so there is kinetic
energy associated with the wave • There is elastic potential energy in the string as it
stretches • The wave carries this energy as it travels • The wave does not carry matter as it travels
• Pieces of the string do not move from one end of the string to the other
Section 12.1
Analysis of The Wave Pulse
• A single pulse propagates to the right
• The graph (part D in the figure shown) shows the displacement of point D on the string • It is perpendicular to
the direction of propagation
• The wave transports energy without transporting matter
Section 12.1
Wave Terminology • The “thing” being disturbed by the wave is its
medium • When the medium is a material substance, the wave
is a mechanical wave • In transverse waves the motion of the medium is
perpendicular to the direction of the propagation of the wave • The string was an example
• In longitudinal waves the motion of the medium is parallel to the direction of the propagation of the wave
Section 12.1
Example: Longitudinal Wave
• The spring is shaken back and forth in the horizontal direction
• At some places the coils are compressed
• At other places the coils are stretched
• This motion produces a longitudinal wave
Section 12.1
Describing Periodic Waves
• Assume a person is shaking the string so that the end is undergoing simple harmonic motion
• The crest is the maximum positive y displacement
• The trough is the maximum negative y displacement
Section 12.2
Periodic vs. Nonperiodic Waves • Nonperiodic waves
• The wave disturbance is limited to a small region of space
• Periodic waves • The wave extends over a very wide region of space • The displacement of the medium varies in a repeating
and often sinusoidal pattern • A periodic wave involves repeating motion as a
function of both space and time
Section 12.2
The Equation of a Wave • Assume the displacement generating the wave in the
string vibrates as a simple harmonic oscillator with yend = A sin (2 π ƒ t)
• The string’s displacement is given by • λ is the symbol for wavelength • This is a mathematical description of a periodic wave • It shows the transverse displacement y of a point on
the string as it varies with time and location
Section 12.2
More Wave Terminology • Periodic waves have a frequency
• The frequency is related to the “repeat time” • The period is the time that a point takes to go from a
crest to the next crest in its motion • Then ƒ = 1 / T
• Periodic waves have an amplitude • Wave crests have y = + A • Wave troughs have y = - A
Section 12.2
Wavelength
• The wavelength is the “repeat distance” of the wave
• Start at a given value of y
• Advance x by a distance equal to the wavelength and y will be at the same value again
Section 12.2
Periodic Wave, Summary • Periodic waves have both a repeat time and a repeat
distance • A periodic wave is a combination of two simple
harmonic motions • One is a function of time • The other is a function of space
Section 12.2
Speed of a Wave • The mathematical description of a wave contains
frequency, wavelength and amplitude • The speed of a wave is
• This is based on the definitions of period and
wavelength
Section 12.2
Direction of a Wave • To determine the direction of the wave, you can focus on
the motion of a crest • As x becomes larger, the wave has moved to the right
and the wave velocity is positive and its equation is
• The equation of a wave moving to the left and having a negative velocity is
Section 12.2
Displacement of the medium as a function of location (x) and time (t)
Amplitude
Frequency
Wavelength
Section 12.2
Interpreting the Equation of a Periodic Wave
Waves on a String • Waves on a string are mechanical waves • The medium that is disturbed is the string • For a transverse wave on a string, the speed of the
wave depends on the tension in the string and the string’s mass per unit length • Mass / length = μ • Tension will be denoted as FT to keep the tension
separate from the period • The speed of the wave is
Section 12.3
Waves on a String, cont. • The speed of the wave is independent of the
frequency of the wave • The frequency will be determined by how rapidly the
end of the string is shaken • The speed of transverse waves on a string is the
same for both periodic and nonperiodic waves
Section 12.3
Sound Waves
• Sound is a mechanical wave that can travel through almost any material • Travels in solids,
liquids, and gases • Assume a speaker is
used to generate the waves
Section 12.3
Sound Waves, cont. • The speaker moves back and forth in the horizontal
direction • As it moves, it collides with nearby air molecules • The x component of the velocity of the air molecules
is affected by the speaker • The displacement of the air molecules associated
with the sound wave is also along the x direction • The result is a longitudinal wave
Section 12.3
Speed of Sound Waves • The speed of sound depends on the properties of
the medium • At room temperature, the speed of sound in air is
approximately 343 m/s • The speed is independent of the frequency • The speed applies to both periodic and nonperiodic
waves • Sound waves in a liquid or solid are also longitudinal • The speed of sound is generally smallest for gases
and highest for solids
Section 12.3
Waves in a Solid
• Solids can support both longitudinal and transverse waves
• The longitudinal waves are considered sound waves
• The speed of the sound depends on the solid’s elastic properties
Section 12.3
Speed of Sound in a Solid • For a thin bar of material, the speed of sound is
given by
• The speed of a transverse wave is more complicated and depends on the shear modulus and other elastic constants
• In general, the speed of the transverse wave is slower than the speed of longitudinal waves
Section 12.3
Transverse Waves • Transverse waves can travel through solids • They cannot travel through liquids or gases
• The displacements in transverse waves involve a shearing motion
• Liquids and gases flow and there is no restoring force to produce the oscillations necessary for a transverse wave
Section 12.3
Electromagnetic Waves • Electromagnetic (em) waves are not mechanical
waves • They are electric and magnetic disturbances that can
propagate even in a vacuum • No mechanical medium is required
• The electric and magnetic fields are always perpendicular to the direction of propagation • So they are transverse waves
• EM waves are classified according to their frequency • The speed of an em wave in a vacuum is 3.00 x 108
m/s • It is independent of the frequency of the wave
Section 12.3
Speed of Waves, Summary • The speed of a wave depends on the properties of
the medium through which it travels • The speed varies widely
• From slow waves on a string • To very fast em waves
• Generally, the wave speed is independent of both frequency and amplitude • There are cases in light and optics where the speed
does depend on the frequency • The speed is the same for periodic and nonperiodic
waves
Section 12.3
Water Waves
• A water wave can be generated by dropping a rock onto the surface
• The waves propagate outward
Section 12.3
Water Waves, cont.
• The motion of the water’s surface is both transverse and longitudinal
• A bug on the surface moves up and down as well as backward and forward
Section 12.3
Wave Fronts: Spherical Waves
• A spherical wave travels away from its source in a three-dimensional fashion
• The wave crests form concentric spheres centered on the source • The crests are also
called wave fronts
Section 12.4
Spherical Waves, cont. • The direction of the wave propagation is always
perpendicular to the surface of a wave front • The direction is indicated by rays • Each wave carries energy as it travels away from the
source • Power measures the energy emitted by the source per
unit time • Units of power are J/s = W • W for Watt
Intensity • Intensity is the power carried by the wave over a unit
area of the wave front • SI units of intensity is W/m2 • Once a wave front is emitted, its energy remains the
same • The intensity falls as the wave moves farther from
the source • The area is becoming larger
Section 12.4
Intensity, cont. • At a distance r from the source, the surface area of
the sphere is 4πr2 • The intensity is
• The intensity falls with distance as
Section 12.4
Plane Waves
• Wave fronts are not always spherical • Another type is a plane wave • In a perfect plane wave, each crest and trough extend over an infinite
plane in space • The intensity is approximately constant over long propagation
distances • Intensity is ideally independent of distance
Section 12.4
Intensity and Amplitude • The intensity of a wave is related to its amplitude
• Spring example
• The potential energy is ½ k x2 • For a wave on a spring, the displacement is
proportional to the amplitude • Therefore, the energy and intensity are proportional to
the square of the amplitude
Section 12.4
Superposition • Waves generally propagate independently of one
another • A wave can travel though a particular region of
space without affecting the motion of another wave traveling though the same region
• This is due to the Principle of Superposition • When two (or more) waves are present, the
displacement of the medium is equal to the sum of the displacements of the individual waves
• The presence of one wave does not affect the frequency, amplitude, or velocity of the other wave
Section 12.5
Constructive Interference
• Two wave pulses are traveling toward each other
• They have equal and positive amplitudes
• At C, the two waves completely overlap and the amplitude is twice the amplitude of the individual waves
• The emerging pulses are unchanged
• This is an example of constructive interference
Section 12.5
Destructive Interference
• Two pulses are traveling toward each other
• They have equal and opposite amplitudes
• At C, the two waves completely overlap, total displacement is zero
• The emerging pulses are unchanged
• This is an example of destructive interference
Section 12.5
Interference • Constructive interference causes the waves to
produce a displacement that is larger than the displacements of either of the individual waves
• Destructive interference causes the waves to produce a displacement that is smaller than the displacements of either of the individual waves
• In either case, the energy of each wave is contained in the kinetic energy of the medium
• The waves can interfere, even destructively, and still carry energy independently
Section 12.5
Interference of Periodic Waves
• The crests of the waves travel away from the initial source • There is constructive interference where the wave crests
overlap • There is destructive interference where a crest and trough
overlap • The result shows an interference pattern with regions of
constructive and destructive interference Section 12.5
Reflection
• Reflection changes the propagation direction of the wave
• Rays can be used to indicate the direction of energy flow
• The rays change direction when a wave reflects from the boundary of the medium
• The wave is inverted as it reflects from a fixed end
Section 12.6
Example: Reflection of Light
• The light wave from a laser reflects from a mirror
Section 12.6
Reflection – Light Ray Details
• The rays make an initial angle of θi with a line drawn perpendicular to the surface
• The perpendicular component of the wave’s velocity reverses direction
• The parallel component of the wave’s velocity is not affected by the reflection
• The angle of incidence will equal the angle of reflection: θi = θr
Section 12.6
Reflection – Free Surface
• The end of the string is attached to a ring that is free to move up and down
• When the wave is reflected, it is not inverted
• The properties of the medium at the boundary will determine if the reflected wave will be inverted or not
Section 12.6
Radar
• An application of wave reflection is radar
• A radio wave pulse is sent from a transmitting antenna and reflects from some distant object
• A portion of the reflected wave will arrive back at the original transmitter, where it is detected
Section 12.6
Radar, cont. • Radar determines the distance to the object by
measuring the time delay between the original and reflected signals
• By using a rotating antenna, the direction of the object can also be detected
• The amplitude of the reflected rays gives information about the size of the object • A larger object reflects more of the wave energy and
gives a larger signal at the detecting antenna
Section 12.6
Refraction
• If the rays follow bent paths in a medium, they are said to be refracted
• The frequency of the wave stays the same • It is determined by the source
• The change in direction of the wave is due to a change in its speed Section 12.7
Standing Waves • Waves may travel back and forth along a string of
length L • If the string has both ends held in fixed positions, the
displacement at both ends must be zero • These conditions can be satisfied by a periodic wave
only for certain wavelengths • For these wavelengths, a standing wave can be
produced • It is called a standing wave because the outline of the
wave appears stationary
Section 12.8
Standing Waves, cont.
• The standing wave is obtained by the interference of two waves traveling in opposite directions
• The waves travel along the string and are reflected from the ends
Section 12.8
Standing Waves, final
• Points where the string displacement is zero are called nodes
• Points where the displacement is largest are called antinodes
• Many standing waves may “fit” into the length of the string
Section 12.8
Harmonics • The longest possible wavelength corresponds to the
smallest possible frequency • This frequency is called the fundamental
frequency, ƒ1 • The next longest wavelength is called the second
harmonic • The pattern of wavelengths and frequencies is
Section 12.8
Harmonics, cont • Combining the frequency and wavelength equations
gives other expressions for the frequency: • This is for standing waves on a string with fixed ends
• The allowed standing wave frequencies are integer multiples of the fundamental frequency
Section 12.8
Musical Tones • Many musical instruments use strings as a vibrating
element • Your fingers press down on the string and changes its
length • The string vibrates with all the possible standing wave
pattern frequencies • The pitch of note is determined by its fundamental
frequency • Two notes whose fundamental frequencies differ by
a factor of 2 are said to be separated by an octave
Section 12.8
Seismic Waves
• Seismic waves propagate through the Earth • Their source can be any large mechanical
disturbance such as an earthquake • There are three types of seismic waves
Section 12.9
Types of Seismic Waves • S waves
• S for shear • Transverse waves • The displacement of the solid Earth is perpendicular to
the direction of propagation • P waves
• P for pressure • Longitudinal sound waves
• Surface waves • Similar to water waves but travel through the surface
of the Earth • Seismic waves can be detected by a seismograph
Section 12.9
Structure of the Earth
• Seismic waves can help determine the interior structure of the Earth
• S waves do not propagate through the core • So the core contains a
liquid • Both S and P waves are
refracted
Section 12.9
Structure of the Earth, cont. • Analysis of the waves led to the following structure:
• Inner core • Outer core • Mantle • Crust
• Many characteristics of these sections also were obtained from the study of seismic waves
Section 12.9