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Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435
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Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Dec 16, 2015

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Page 1: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Chapter 14Waves and sound

Dr. Haykel Abdelhamid Elabidi

November/December 2013/Muh 1435

Page 2: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Units of Chapter 14

• Types of waves• Harmonic wave functions • Waves on a string• Sound waves• Sound intensity• Superposition and interference• Standing waves

Page 3: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Types of wavesA wave is a disturbance that propagates from one place to another.

1. Transvers wave: the displacement of the medium is perpendicular to the direction of motion of the wave.

The wave on a string have the shape of sine or cosine; such a waves are called harmonic wave.

2. Longitudinal wave: the displacement of individual particles is parallel to the direction of propagation of the wave.

The individual particle in the air oscillate back and forth about a given position.

3. Water waves: are a combination of transverse and longitudinal waves

Page 4: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Types of waves

Transvers wave

Longitudinal wave

Page 5: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Types of waves

The period T is the time for one wavelength to pass a given point.

The wavelength λ is the distance over which the wave repeats.

Page 6: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Types of waves

Exercise 2: A tennis ball is hit back and forth between two players warming up for a match, If it takes 2.31 s for the ball to go from one player to the other. What are the period and the frequency of the ball’s motion?

Solution:

Page 7: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

The harmonic wave functions

Exercise:

Solution:

Page 8: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Waves on a string

Page 9: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Waves on a string

When a wave reaches the end of a string, it will be reflecte. If the end is fixed, the reflected wave will be inverted.

If the end of the string is free to move transversely, the wave will be reflected without inversion

Page 10: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Sound waves

The human ear can hear sounds between about 20 Hz and 20 KHzf<20 Hz: Infrasonicf>20 KHz:Ultrasonic

Page 11: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Sound waves

Page 12: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Sound intensity• The loudness of a sound is defined by its intensity.• The intensity of a sound is the amount of energy that passes through a

given area in a given time:

Page 13: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Sound intensity

Page 14: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Sound intensity

• The loudness of a sound doubles with each increase in intensity level by 10dB

Page 15: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Superposition and interference

The superposition is a combination of a two or more waves to form a result wave

Part A: Superposition

Page 16: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Superposition and interference

• Constructive interference: if two pulses combine to give a large pulse

• Destructive interference: if two pulses combine to give a smaller pulse

Part B: Interference

Page 17: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Superposition and interference

• Two sources 1 and 2 are emitting sound to a point A:

Two waves in phase Two waves have opposite phase

Page 18: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Superposition and interference

Page 19: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Superposition and interference

Calculate the path length difference

Page 20: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Superposition and interference

Solution:

Page 21: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Superposition and interference

Page 22: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Standing waves

A standing wave is the wave that is fixed in its location but oscillates with time.

These waves are found on strings with both ends fixed, such as in a musical instrument or in vibrating columns of air (like a soda bottles)

Page 23: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Standing waves

Page 24: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Standing waves

The fundamental, or lowest, frequency on a fixed string has a wavelength twice the length of the string.

chap14-Wave Reflection and Standing Waves 2.mp4 - YouTube.FLV

Page 25: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Standing waves

Higher frequencies are called harmonics

Points on the string which never move are called nodes (N); those which have the maximum movement are called antinodes (A).

Page 26: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Standing waves

Page 27: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Standing waves

Standing waves can also be excited in columns of air, such as soda bottles (closed at one end).

One end (closed) is a node (N), and the other (open) is an antinode (A).

Page 28: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Standing waves

Only odd-numbered harmonics appear: 1st, 3nd, 5rd,….

Summary:

Page 29: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Standing waves

Page 30: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Standing waves

If the tube is open at both ends, both ends are antinodes, and the sequence of harmonics is the same as that on a string.

Page 31: Chapter 14 Waves and sound Dr. Haykel Abdelhamid Elabidi November/December 2013/Muh 1435.

Thank you for your attention

See you next time Inchallah