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WAVES AT MEDIA BOUNDARIES Section 9.2
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WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms Media Boundary Free-end Reflection Fixed-end Reflection Transmission Standing Wave Node

Apr 01, 2015

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Page 1: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

WAVES AT MEDIA BOUNDARIES

Section 9.2

Page 2: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Key Terms

Media Boundary Free-end Reflection Fixed-end Reflection Transmission Standing Wave Node Antinode Fundamental Frequency/First

Harmonic Harmonics Overtone

Page 3: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Media Boundaries

Wave speed depends on the properties of the medium through which the wave is travelling.

All media have boundaries. The location where two media meet.

Page 4: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Free-End Reflections

If a wave travels from a more dense medium to a less dense medium, it will travel more quickly in the more dense medium. Wave moving towards the boundary will be

reflected with the same orientation and amplitude

Page 5: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Fixed-End Reflection

As a wave moves towards a fixed boundary, it will reflect. Reflected pulse has the

same shape as the incoming pulse, but its orientation is inverted.

Page 6: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Amplitude

When a wave encounters a boundary that is not strictly free-end or fixed-end, the wave will split in two. One wave is reflected

Energy “bounces back”. The other is transmitted.

Energy passes into new medium. Amplitude of the two waves may not be

equal, but the sum of the amplitudes will be equal to that of the original wave.

Page 7: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Media Boundaries

Not all difference in media boundaries are as dramatic as fixed-end or free-end. Water Air

If a wave travels from a medium in which the speed is faster (more dense) to a medium in which the speed is slower (less dense), the wave particles can move more freely Energy is transferred

into new medium Reflected wave has

same orientation

Page 8: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Media Boundaries

The opposite is also true. Air Water

If a wave travels from a medium in which the speed is slower (less dense) to a medium in which the speed is faster (more dense), the wave particles cannot move as freely Energy is transferred

into new medium Reflected wave has

inverted orientation

Page 9: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Standing Waves

Suppose a series of waves is sent down a string that is fixed at both ends. At a certain frequency, reflected waves will

superimpose on the stream of incoming waves to produce waves that appear stationary

The locations in which the particles of the medium do not move are nodes.

The locations in which the particles of the medium move with the greatest speed are antinodes.

Page 10: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Standing Wave

Page 11: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Standing Waves

Waves interfere according to principle of superposition. Waves are moving continuously At the antinodes, the amplitudes of the

troughs and crests are double that of the original wave.

At the nodes, the amplitudes are the same but one is a crest and the other is a trough. Interference pattern appears to be stationary

because it is produced by otherwise identical waves travelling in opposite directions.

Page 12: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Standing Waves Between Two Fixed Ends

Standing waves can be predicted mathematically. Consider a string with two fixed ends

Standing wave with nodes at both ends. The shortest length of the string, L, is equal to

one half of the wavelength. The frequency of the wave that produces this

simplest standing wave is called the fundamental frequency

First harmonic All standing waves to follow require frequencies

that are whole-number multiples of the fundamental frequency.

Additional standing wave frequencies are known as the nth harmonic of the fundamental frequency

Page 13: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Symbol Number of Nodes Between Ends

Diagram Harmonic (n) Overtone

f0 0 First Fundamental

f1 1 Second First

f2 2 Third Second

f 3 Fourth Third

Page 14: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Harmonics and Overtones

Harmonics consist of the fundamental frequency of a musical sound as well as the frequencies that are the whole-number multiples of the first harmonic.

When a string vibrates with more than one frequency, the resulting sounds are called overtones. Similar to harmonics, however the first

overtone is equal to the second harmonic.

Page 15: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Calculations with Standing Waves The length of the medium is equal to the

number of the harmonic times half the standing wave’s length.

For a media with a combination of fixed and free ends (node at one end and antinode at the other), the equation is:

Page 16: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node
Page 17: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node
Page 18: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node
Page 19: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Summary

Page 20: WAVES AT MEDIA BOUNDARIES Section 9.2. Key Terms  Media Boundary  Free-end Reflection  Fixed-end Reflection  Transmission  Standing Wave  Node

Homework

Page 426 Questions 1-5