Title: Waves and Sound
1Chapter 14
2Wave Motion
- A wave is a moving self-sustained disturbance of
a medium either a field or a substance. - Mechanical waves are waves in a material medium.
- Mechanical waves require
- Some source of disturbance
- A medium that can be disturbed
- Some physical connection between or mechanism
though which adjacent portions of the medium
influence each other - All waves carry energy and momentum
3Wave Characteristics
- The state of being displaced moves through the
medium as a wave. - A progressive or travelling wave is a
self-sustaining disturbance of a medium that
propagates from one region to another, carrying
energy and momentum. - Examples waves on a string, surface waves on
liquids, sound waves in air, and compression
waves in solids or liquids. - In all cases the disturbance advances and not the
medium.
4Traveling Waves
- Flip one end of a long rope that is under tension
and fixed at one end - The pulse travels to the right with a definite
speed - A disturbance of this type is called a traveling
wave
5Description of a Wave
- A steady stream of pulses on a very long string
produces a continuous wave - The blade oscillates in simple harmonic motion
- Each small segment of the string, such as P,
oscillates with simple harmonic motion
6Amplitude and Wavelength
- Amplitude (A) is the maximum displacement of
string above the equilibrium position - Wavelength (?), is the distance between two
successive points that behave identically
7Longitudinal Waves
- In a longitudinal wave, the elements of the
medium undergo displacements parallel to the
motion of the wave - A longitudinal wave is also called a compression
wave
8Longitudinal Wave Represented as a Sine Curve
- A longitudinal wave can also be represented as a
sine curve - Compressions correspond to crests and stretches
correspond to troughs - Also called density waves or pressure waves
9Transverse Waves
- In a transverse wave, each element that is
disturbed moves in a direction perpendicular to
the wave motion
10Waveforms
- Wavepulse in taut rope. Shape of pulse is
determined by motion of driver. - If driver (hand) oscillates up and down in a
regular way, it generates a wave train a
constant frequency carrier whose amplitude is
modulated (varies with time.)
11Waveform The shape of a Wave
- The high points are crests of the wave
- The low points are troughs of the wave
- As a 2-D or 3-D wave propagates, it creates a
wavefront
12Velocity of Waves
- Period (T) of a periodic wave - time it takes for
a single profile to pass a point in space - the
number of seconds per cycles. - The inverse of the period (1 /T) is the frequency
f, the number of profiles passing per second, the
number of cycles per second. - The distance in space over which the wave
executes one cycle of its basic repeated form is
the wavelength, l the length of the profile.
13Velocity of Waves
- The speed of the wave the rate (in m/s) at
which the wave advances - Is derived from the basic speed equation of
distance/time - Since a length of wave l passes by in a time T,
its speed must equal l /T f l - The speed of any progressive periodic wave
- v fl
14Example 1
- A youngster in a boat watches waves on a lake
that seem to be an endless succession of
identical crests passing, with a half-second
between them. If one wave takes 1.5 s to sweep
straight down the length of her 4.5 m-long boat,
what are the frequency, period, and wavelength of
the waves? - Given The waves are periodic 0.5 s between
crests L 4.5 m t 1.5 s - Find T, f, v, and l
15Transverse Waves Strings
- The speed of a mechanical wave is determined by
the inertial and elastic properties of the medium
and not in any way by the motion of the source - Pulse traveling with a speed v along a
lightweight, flexible string under constant
tension FT - v (11.3)
- When m/L is large, there is a lot of inertia and
the speed is low. When FT is large, the string
tends to spring back rapidly, and the speed is
high
16Example 2
- A 2.0 m-long horizontal string having a mass of
40 g is slung over a light frictionless pulley,
and its end is attached to a hanging 2.0 kg mass.
Compute the speed of the wavepulse on the
string. Ignore the weight of the overhanging
length of rope. - Given A string of length l 2.0 m, m 40 g
supporting a 2.0 kg load - Find v
17Reflection, Refraction, Diffraction and Absorption
- End of rope is held stationary energy pumped in
at the other end, the reflected wave ideally
carries away all the original energy - It is inverted 180 out-of-phase with the
incident wave - End of the rope is free it will rise up as the
pulse arrives until all the energy is stored
elastically. - The rope then snaps back down, producing a
reflected wavepulse that is right side up.
18Reflection of Waves Fixed Boundary
- Whenever a traveling wave reaches a boundary,
some or all of the wave is reflected - When it is reflected from a fixed end, the wave
is inverted - The shape remains the same
19Reflected Wave Open Boundary
- When a traveling wave reaches an open boundary,
all or part of it is reflected - When reflected from an open boundary, the pulse
is not inverted
20Reflection, Refraction, Diffraction and Absorption
- When a wave passes from one medium to another
having different physical characteristics, there
will be a redistribution of energy. - Medium is also displaced, and a portion of the
incident energy appears as a refracted wave. - If the incident wave is periodic, the transmitted
wave has the same frequency but a different speed
and therefore a different wavelength the larger
the density of the refracting medium, the smaller
the length of the wave.
21Reflection, Refraction, Diffraction and Absorption
- When a wave meets a hole or another obstacle, it
can be bent around it or through itDiffraction - A wave can lose part or all of its energy when it
meets a boundary Absorption.
22Reflection, Refraction, Diffraction and Absorption
- A wave passing through a lens will be both
reflected AND refracted. Examples include light
(of course) and also sound (through the balloon
of different gas) - Absorption can either SUBTRACT (beach sand) or
ADD (wind) energy to a wave, depending on which
way the energy is being transferred.
23Superposition of Waves
- Superposition Principle In the region where two
or more waves overlap, the resultant is the
algebraic sum of the various contributions at
each point. - Superimposing two harmonic waves of the same
frequency and amplitude at every value of x, add
the heights of the two sine curves above the
axis as positive and below it as negative. - The sum of any number of harmonic waves of the
same frequency traveling in the same direction is
also a harmonic wave of that frequency.
24Interference of Waves
- Two traveling waves can meet and pass through
each other without being destroyed or even
altered - Waves obey the Superposition Principle
- If two or more traveling waves are moving through
a medium, the resulting wave is found by adding
together the displacements of the individual
waves point by point - Actually only true for waves with small amplitudes
25Constructive Interference
- Two waves, a and b, have the same frequency and
amplitude - Are in phase
- The combined wave, c, has the same frequency and
a greater amplitude
26Destructive Interference
- Two waves, a and b, have the same amplitude and
frequency - They are 180 out of phase
- When they combine, the waveforms cancel
27Superposition
- When two or more waves interact, their
amplitudes are added (superimposed) one upon the
other, creating interference. - Constructive interference
- occurs when the superposition
- increases amplitude.
- Destructive interference
- occurs when the superposition
- decreases the amplitude.
28Natural Frequency/Harmonics
- If a periodic force occurs at the appropriate
frequency, a standing wave will be produced in
the medium. -
- The lowest natural frequency in a medium is its
fundamental harmonic. - Double this frequency to produce the 2nd
harmonic. - Triple this frequency to produce the 3rd harmonic
29Natural Frequency/Harmonics
REQUIRES FIXED BOUNDARIES
30Frequency and Period
- w0 - the natural angular frequency, the specific
frequency at which a physical system oscillates
all by itself once set in motion - natural angular frequency
- and since w0 2pf0
- natural linear frequency
- Since T 1/f0
- Period
31Waves and Energy
- As waves propagate, their energy alternates
between two froms - Transverse Waves Potential ltgt Kinetic
- Longitudinal Waves Pressure ltgt Kinetic
- Light Waves Electric ltgt Magnetic
32Waves and Energy
-
- Generally
- HIGHER FREQUENCY HIGHER ENERGY
- HIGHER AMPLITUDE HIGHER ENERGY
33Nodes and Modes
- Nodes occur/are located at points of
equilibrium within a wave. - Anitnodes occur/are located at points of
greatest displacement (amplitude) within a wave.
34Nodes and Modes
- One-dimensional modes
- Transverse guitar or piano strings
- Rotational jump rope, lasso
- Two- and Three-dimensional modes
- Radial concentric circular nodes and anti-nodes
- Angular linear nodes and anti-nodes radiating
outward from center.
35Nodes and Modes
36Nodes and Modes