Chapter13 MJM s7 9 Sound

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Today 2/24/14 Read Chapter 13.7 to 13.9 (p455 to 461) Watch the rest of this presentation Complete ex ample problems in the book Complete HW  Given at the end of the presenta tion

Transcript of Chapter13 MJM s7 9 Sound

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Today 2/24/14

• Read Chapter 13.7 to 13.9 (p455 to 461)

• Watch the rest of this presentation

• Complete example problems in the book• Complete HW

– Given at the end of the presentation

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Raymond A. Serway

Chris Vuille

Chapter ThirteenVibrations and Waves

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Wave Motion

• A wave = the motion of a disturbance

• Mechanical waves require – Source of disturbance

– A medium that can be disturbed – Some physical connection within the medium which allows

influence to the rest of the medium

• All waves carry energy and momentum

Section 13.7

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Types of Waves – Traveling Waves

• Flip one end of a long rope thatis under tension and fixed at theother end

• The pulse travels to the rightwith a definite speed• A disturbance of this type is

called a traveling wave

Section 13.7

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Types of Waves – Transverse

• Transverse wave = each element disturbed moves in adirection perpendicular to the wave motion

Section 13.7

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Video of Transverse Wave

• https://www.youtube.com/watch?v=AtlxBODxWHc

• https://www.youtube.com/watch?v=Rbuhdo0AZDU

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Types of Waves – Longitudinal

• Longitudinal wave = elements of the medium aredisplaced parallel to the motion of the wave

• Also called a compression wave

Section 13.7

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Videos of Longitudinal Wave

• https://www.youtube.com/watch?v=ubRlaCCQfDk

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Waveform – A Picture of a Wave

• The brown curve is a“snapshot” of the wave atsome instant in time

• The blue curve is the samewave at a later time

• The high points are crests

• The low points are troughs

Section 13.7

Crest

Trough

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Longitudinal Wave Represented as a Sine Curve

• A longitudinal wave can also be represented as a sine curve• Compressions of coils correspond to crests

• Stretches areas of coil correspond to troughs• Also called density waves or pressure waves

Section 13.7

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Producing Waves

Section 13.8

• The blade vibrates causingoscillates in simple harmonicmotion in the string

• A steady stream of pulses on avery long string produces acontinuous wave

• Each small segment of the string,

such as P, oscillates with simpleharmonic motion

Blade

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Amplitude and Wavelength

• Amplitude = maximumdisplacement of string abovethe equilibrium position

• Wavelength (λ) = distancebetween two successivepoints that behave identically

• Period (T) = time it takes tomove through one cycle

• Frequency (ƒ) = vibrations perunit time (ƒ=1/T)

Section 13.8

Δy = amplitude Δx = wavelength

Equilibrium (X=0)

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Speed of a Wave on a String

• The speed on a wave stretched under sometension, F

– v = velocity (speed) – F = force (tension in the string)

– m is called the linear density (mass/unit Length)

• The speed depends only upon the propertiesof the medium – Ex: a denser medium will have less speed

Section 13.9

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Example Problems

• Now go back to the book and look overExample Problems 13.8, 13.9, 13.10

• This will prepare you to do your homework

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