1. Physics 260 Conceptual discussion of wave motion Wave properties
Mathematical description
Waves on a string

2. What is a wave ? Examples: Sound waves (air moves back & forth)
:A wave is a traveling disturbance that transports energy but not matter.
Examples:
Sound waves (air moves back & forth)
Stadium waves (people move up & down)
Water waves (water moves up & down)
Light waves (what moves??)

3. Characteristics of Wave Motion
Where do Waves come from and what are Periodic Waves? waves in mechanical media.
Wave types
Transverse and Longitudinal
Energy transported by Waves
How do waves Transmit Energy?
Mathematical representation of a traveling wave
The Principle of Superposition
Interference Standing Waves: Resonances

4. Types of Waves
Transverse: The medium oscillates perpendicular to the direction the wave is moving.
Water
Slinky
Longitudinal: The medium oscillates in the same direction as the wave is moving
Sound
Slinky waves-tr-long

5. Figure 15-5

6. Figure 15-2

7. Figure 15-6

8. Figure 15-10

9. Wave Forms v
So far we have examined “continuous waves” that go on forever in each direction! v
We can also have “pulses” caused by a brief disturbance of the medium: v
And “pulse trains” which are somewhere in between.

10. Figure 15-3

11. Mathematical Descriptionx y
Suppose we have some function y = f(x):
f(x - a) is just the same shape moved a distance a to the right: x y
x = a
Let a = vt Then
f(x - vt) will describe the same shape moving to the right with speed v.
traveling waves properties x y
x = vt v

12. Periodic Wave Properties
Wavelength
Wavelength: The distance  between identical points on the wave.
Amplitude A
Amplitude: The maximum displacement A of a point on the wave. A

13. Wave Properties...
Period: The time T for a point on the wave to undergo one complete oscillation.
Speed: The wave moves one wavelength  in one period T so its speed is v = / T.

14. Math... y 
Consider a wave that is harmonic in x and has a wavelength of . A x
If the amplitude is maximum at x = 0 this has the functional form: v y
Now, if this is moving to the right with speed v it will be described by: x

15. Math...
So we see that a simple harmonic wave moving with speed v in the x direction is described by the equation:
By using
from before, and by defining
we can write this as:
(what about moving in the -x direction?)

16. Figure 15-7

17. Math Summary y 
The formula describes a harmonic wave of amplitude A moving in the +x direction. A x
Each point on the wave oscillates in the y direction with simple harmonic motion of angular frequency .
The wavelength of the wave is
The speed of the wave is
The quantity k is often called the “wave number”

18. Wave Properties...
v =  / T
We will show that the speed of a wave is a constant that depends only on the medium, not on amplitude, wavelength, or period  and T are related!
 = v T or  = 2 v / (sinceT = 2 /  or  = v / f (since T = 1 / f ) 

19. Waves on a string What determines the speed of a wave?
Consider a pulse propagating along a string: v

20. Waves on a string... Suppose: The tension in the string is F
The mass per unit length of the string is  (kg/m)
The shape of the string at the pulse’s maximum is circular and has radius R F  R

21. Waves on a string... Consider moving along with the pulse
Apply F = ma to the small bit of string at the “top” of the pulse v x y

22. Waves on a string... So we find: v tension F mass per unit length 
Making the tension bigger increases the speed.
Making the string heavier decreases the speed.
As we asserted earlier, this depends only on the nature of the medium, not on amplitude, frequency, etc. of the wave.

23. Wave Power
A wave propagates because each part of the medium communicates its motion to adjacent parts.
Energy is transferred since work is done!
How much energy is moving down the string per unit time.
(i.e. how much power?) P

24. Wave Power...
Think about grabbing the left side of the string and pulling it up and down in the y direction.
You are clearly doing work since F.dr > 0 as your hand moves up and down.
This energy must be moving away from your hand (to the right) since the kinetic energy (motion) of the string stays the same. P

25. How is the energy moving?
Consider any position x on the string. The string to the left of x does work on the string to the right of x, just as your hand did: x  F
Power P = F.v v x

26. Power along the string If  x F v  Recall sin    cos   1
Since v is along the y axis only, to evaluate Power = F.v we only need to find Fy = -F sin   -F  if  is small. We can easily figure out both the velocity v and the angle  at any point on the string: If y  Fy x F v dy  dx
Recall
sin   
cos   1
for small 
tan   

27. Power...
So:
But last time we showed that and

28. Average Power
We just found that the power flowing past location x on the string at time t is given by:
We are often just interested in the average power moving down the string. To find this we recall that the average value of the function sin2 (kx - t) is 1/2 and find that:
It is generally true that wave power is proportional to the speed of the wave v and its amplitude squared A2.

29. Energy of the Wave We have shown that energy “flows” along the string.
The source of this energy (in our picture) is the hand that is shaking the string up and down at one end.
Each segment of string transfers energy to (does work on) the next segment by pulling on it, just like the hand.
We found that So
is the average energy per unit length.

30. Recap & Useful Formulas:y  A x
General harmonic waves
Waves on a string
tension
mass / length

31. Superposition Q: What happens when two waves “collide?”
A: They ADD together!
We say the waves are “superposed.”

32. Figure (a)

33. Figure (b)

34. Figure (b)

35. Superposition & Interference
We have seen that when colliding waves combine (add) the result can either be bigger or smaller than the original waves.
We say the waves add “constructively” or “destructively” depending on the relative sign of each wave.
will add constructively
will add destructively
In general, we will have both happening

36. Superposition & Interference
Consider two harmonic waves A and B meeting at x=0.
Same amplitudes, but 2 = 1.15 x 1.
The displacement versus time for each is shown below:
A(1t)
B(2t)
What does C(t) = A(t) + B(t) look like??

37. Figure (a)

38. Figure (b)

39. Figure (c)

40. Interference
Interference: Combination of two or more waves to form composite wave –use superposition principle.
Waves can add constructively or destructively
Conditions for interference:
1.Coherence: the sources must maintain a constant phase with respect to each other
2.Monochromaticity: the sources consist of waves of a single wavelength

45. Superposition & Interference
Consider two harmonic waves A and B meeting at x = 0.
Same amplitudes, but 2 = 1.15 x 1.
The displacement versus time for each is shown below:
A(1t)
B(2t)
CONSTRUCTIVE INTERFERENCE
DESTRUCTIVE INTERFERENCE
C(t) = A(t) + B(t)

46. Beats Can we predict this pattern mathematically? Of course!
Just add two cosines and remember the identity:
where
and
cos(Lt)

50. Figure 15-41
Problem 73.

53. Figure 15-26

54. Figure (a)

55. Figure 15-28
Example 15-8.

56. Figure 15-40
Problem 71.

57. Physics for Scientists & Engineers, 3rd Edition
Douglas C. Giancoli
Chapter 16
Sound
© Prentice Hall

58. Figure 16-1
Example 16-2

59. Figure 16-2

60. Figure 16-3

61. Figure 16-4 characteristic of sound 1 HyperPhysics Concepts
Maximum Sensitivity Region of Human Hearing
Equal Loudness Curves
Speed of Sound

62. intensity of sound, decibels 3
Sound Intensity
Decibels
Examples of Sound Level Measurements

63. Figure 16-5

64. Sources of sound, vibrating string and air columns
Standing Waves on a String
Resonances of open air columns
Resonances of closed air columns
Longitudinal Waves - Kundt's Tube
Fundamental and Harmonic Resonances

66. Figure (b)

70. Figure 16-7

71. Figure 16-8

72. Figure (a)

73. Figure (b)

74. Figure (a)

75. Figure (b)

76. Figure 16-15

77. Figure 16-16

78. Figure 16-17

79. Figure 16-18

80. No motion λ produced =λ’heard

81. Source moving Figure 16-19 (b)

82. Source moving towards observer λobserved = λproduced (1-v source /v sound) fobserved = f produced/(1-v source /v sound)

83. Observer moving towards source fobserved = f produced(1+v source /v sound)

84. Doppler effect 7
The Doppler Effect for Sound
The  Doppler Effect for Sound
Police RADAR
Doppler Pulse Detection

85. Figure 16-22
Example

86. Figure 16-26

87. Figure (a)

88. Figure 16-33
Problem 52.

89. Figure 16-36
Problem 86.

90. Figure 16-38
Problem 96.

91. Figure 16-39
Problem 101.

92. Figure 16-40
Problem 102.