Wave Motion

6,426 views 33 slides Oct 06, 2015
Slide 1
Slide 1 of 33
Slide 1
1
Slide 2
2
Slide 3
3
Slide 4
4
Slide 5
5
Slide 6
6
Slide 7
7
Slide 8
8
Slide 9
9
Slide 10
10
Slide 11
11
Slide 12
12
Slide 13
13
Slide 14
14
Slide 15
15
Slide 16
16
Slide 17
17
Slide 18
18
Slide 19
19
Slide 20
20
Slide 21
21
Slide 22
22
Slide 23
23
Slide 24
24
Slide 25
25
Slide 26
26
Slide 27
27
Slide 28
28
Slide 29
29
Slide 30
30
Slide 31
31
Slide 32
32
Slide 33
33

About This Presentation

Wave motion Chapter for 12


Slide Content

Wave Motion

What’s the first thing that comes to mind when you hear the word “wave”? We often think of common forms of waves such as the waves in the ocean . But there are many kinds of waves. Waves are all around us and we encounter them everyday. There are light waves, sound waves, and many more. In this section, we are going to look at common types of waves , what parts make up those waves, and real life examples of waves. Introduction to Waves

Amplitude is a measurement from equilibrium to the crest of a wave. Equilibrium is the point half way in between a crest and a trough in the vertical direction. We measure to the crest instead of the trough because then the amplitude is a positive number. Amplitude is a measure of the intensity of a wave. The symbol for amplitude is A and it is measured in meters. Amplitude

The wavelength is the length of one complete wave, or cycle. It is measured from crest to crest or from trough to trough for transverse waves . It is similar for longitudinal waves as well. The symbol for wavelength is the Greek letter lambda ( λ ) and is measured in meters. Wavelength

Period Period is the time it takes to complete one full cycle of a wave. A cycle is from rarefaction to rarefaction or from compression to compression for longitudinal waves . It is similar for transverse waves as well. The symbol for period is T and it is measured in seconds.

Frequency is the number of cycles that occur for every unit of time. There are two equations for frequency. These are used to make calculations with waves. The symbol for frequency if f and it is measured in cycles per second. Frequency f = ─ T 1 f = ─ v λ Frequency is the inverse of period : Frequency is equal to the velocity of a wave divided by the wavelength :

The crest is the highest point in the vertical direction for a transverse wave . Similarly, the trough is the lowest point in the vertical direction. Crests and Troughs

The compression of a longitudinal wave is the part of the wave where the particles in a wave are most dense. Rarefaction is the part of the wave where the particles are least dense. Compression and Rarefaction

There are many types of waves. In this section, we’re specifically going to look at transverse waves and longitudinal waves , as well as examine a special type of wave called a standing wave . They are examples of mechanical waves. An important concept about wave motion is that waves transfer energy, NOT matter. Types of Waves

A transverse wave is characterized by particle motion that is perpendicular to the wave energy. It is important to understand that an individual particles do not move from there original position on the horizontal axis, they merely oscillate vertically. Transverse Waves Click on the picture to visit a website that let’s you adjust the wavelength and amplitude of a transverse wave.

A longitudinal wave is characterized by particle motion that is parallel to the direction of the wave energy. Even though they are in the same direction, it is important to note that a particle does not move with the wave, it merely oscillates in the same direction. Longitudinal Waves Click on the picture to visit a website that shows animated pictures of wave motion.

The simplest type of wave is the one in which the particles of the medium are set into simple harmonic vibrations as the wave passes through it. The wave is then called a simple harmonic wave. Consider a particle O in the medium. The displacement at any instant of time is given by

Where A is the amplitude, w is the angular frequency of the wave. Consider a particle P at a distance x from the particle O on its right. Let the wave travel with a velocity v from left to right. Since it takes some time for the disturbance to reach P, its displacement can be written as

Where f is the phase difference between the particles O and P. We know that a path difference of l corresponds to a phase difference of 2p radians. Hence a path difference of x corresponds to a phase difference of  2 π x ʎ Substituting equation (1.5) in equation (1.4) We get,         

                                                                                                                                                                                                                                                                                                                                                                                 Similarly, for a particle at a distance x to the left of 0, the equation for the displacement is given by                                                                                                            

16 Boundary Behavior The behavior of a wave when it reaches the end of its medium is called the wave’s BOUNDARY BEHAVIOR . When one medium ends and another begins, that is called a boundary .

17 Fixed End One type of boundary that a wave may encounter is that it may be attached to a fixed end . In this case, the end of the medium will not be able to move. What is going to happen if a wave pulse goes down this string and encounters the fixed end?

18 Fixed End Here the incident pulse is an upward pulse. The reflected pulse is upside-down. It is inverted. The reflected pulse has the same speed , wavelength , and amplitude as the incident pulse.

19 Fixed End Animation

20 Free End Another boundary type is when a wave’s medium is attached to a stationary object as a free end . In this situation, the end of the medium is allowed to slide up and down. What would happen in this case?

21 Free End Here the reflected pulse is not inverted. It is identical to the incident pulse, except it is moving in the opposite direction. The speed , wavelength , and amplitude are the same as the incident pulse.

22 Free End Animation

23 Change in Medium Our third boundary condition is when the medium of a wave changes. Think of a thin rope attached to a thin rope. The point where the two ropes are attached is the boundary. At this point, a wave pulse will transfer from one medium to another. What will happen here?

24 Change in Medium In this situation part of the wave is reflected, and part of the wave is transmitted. Part of the wave energy is transferred to the more dense medium, and part is reflected. The transmitted pulse is upright, while the reflected pulse is inverted.

25 Change in Medium The speed and wavelength of the reflected wave remain the same, but the amplitude decreases. The speed , wavelength , and amplitude of the transmitted pulse are all smaller than in the incident pulse.

26 Change in Medium Animation

27 Wave Interaction All we have left to discover is how waves interact with each other. When two waves meet while traveling along the same medium it is called INTERFERENCE .

28 Constructive Interference Let’s consider two waves moving towards each other, both having a positive upward amplitude. What will happen when they meet?

29 Constructive Interference They will ADD together to produce a greater amplitude. This is known as CONSTRUCTIVE INTERFERENCE .

30 Destructive Interference Now let’s consider the opposite, two waves moving towards each other, one having a positive (upward) and one a negative (downward) amplitude. What will happen when they meet?

31 Destructive Interference This time when they add together they will produce a smaller amplitude. This is know as DESTRUCTIVE INTERFERENCE .

32 Check Your Understanding Which points will produce constructive interference and which will produce destructive interference ? Constructive G, J, M, N Destructive H, I, K, L, O

Quickne tube Experiment