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Chapter 15 Wave Motion

Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

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Page 1: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Chapter 15

Wave Motion

Page 2: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Section 15-1: Simple Wave Motion

Transverse and Longitudinal Waves

A transverse wave

Page 3: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

The oscillation of a transverse wave is perpendicular to the wave motion.

Page 4: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

A longitudinal wave

The oscillation of a spring is parallel to the motion

Page 5: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Wave pulses

A wave pulse is a travelling disturbance.

Page 6: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

The speed of waves

The speed of a wave is a property of the medium in which it travels.

In a stretched string v= (F/μ)½

In a fluid v= (B/ρ)½

And in a gas v=(γRT/M)½

The are called the dispersion relations for the media.

Page 7: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

The derivation of v for waves on a string

Page 8: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

The Wave Equation

ð2y/ðx2 = (1/v2) ð2y/ðt2

Here y represents the vertical displacement of the string. It is called the wave function

Page 9: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Section 15-2: Harmonic Waves

Harmonic waves on a string have a wave function of the form y=Asin(kx-ωt+φ).

Page 10: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

The Energy of Waves on a String

Page 11: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave
Page 12: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Harmonic Sound Waves

Sound waves have a wave

function of the form:

s=s0sin(kx-ωt) where s

represents the horizontal

displacement of the wave.

The Energy of Sound Waves

Page 13: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Electromagnetic Waves: These will be studied in Phy 2049

Section 15-3: Waves in Three Dimensions

Circular wavefronts

Page 14: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave
Page 15: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Sound waves from a telephone handset.

Page 16: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

At a great distance from the source, spherical wavefronts look like parallel planes called plane waves

Page 17: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

A two dimensional analog to plane waves

Page 18: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Wave Intensity

Wave intensity is the radiated power per unit area of the wavefront.

Page 19: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Intensity Level and Loudness: This would be equivalent to brightness in a light wave.

β = 10 log (I/I0) in decibels (dB). I0 is the threshold of hearing= 1x10-12 watts/m2

Section 15-4: Waves Encountering Barriers

Reflection and Refraction: Reflection is the “bouncing” of a wave incident on an interface, back into the same medium

Page 20: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Refraction is the “bending” of the path of a light ray as it travels from one medium into another. This is due to a difference in wave speed between the two media.

Page 21: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Total Internal Reflection is when an incident ray is totally internally reflected. This occurs when the angle of incidence is a critical value.

Page 22: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave
Page 23: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

A wave from a light string encountering a heavier string (for which the speed is lower) suffers a phase change of π upon reflection.

Page 24: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

A wave from a heavy string encountering a lighter string (for which the speed is higher) suffers no phase change.

Page 25: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Tunneling is when a wave penetrates through a barrier.

Page 26: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Diffraction: The ability of a wave to move around an obstacle in its path.

Waves in a ripple tank encountering a wall with a slit. If the slit width is small compared to λ, the waves move in around the barrier and the slit becomes a point source.

Page 27: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

If the slit width is large compared to λ, there is very little diffraction.

Page 28: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Transmitted waves radiate widely as they pass through a slit. The slit acts as a point source.

Transmitted particles are confined to narrow angle.

Page 29: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Sound waves can give images, just like light.

Page 30: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Section 15-5: The Doppler Effect

The Doppler Effect is a shift in frequency of a wave when there relative motion between the source and the observer. The shift is toward higher frequencies (shorter wavelengths) when the source and observer are approaching, and to lower frequencies (longer wavelengths) when they are receding.

Page 31: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave
Page 32: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

Shock Waves

When the source is traveling faster than the speed of the sound wave in the medium, shock waves result when the waves interfere with each other.

Page 33: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave
Page 34: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

This is the reason for the “sonic boom” produced by jets that exceed the sound barrier.

Page 35: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

This is “bow shock”.

Page 36: Chapter 15 4 Wave Motion. Section 15-1: Simple Wave Motion Transverse and Longitudinal Waves A transverse wave

When applied to electromagnetic waves, this is called the Cerenkov Effect.