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Fall 2004 Physics 3 Tu-Th Section - hep.ucsb.eduhep.ucsb.edu/people/claudio/ph3-04/lecture1.pdf ·...

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1 Fall 2004 Physics 3 Tu-Th Section Claudio Campagnari Web page: http://hep.ucsb.edu/people/claudio/ph3-04/
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Page 1: Fall 2004 Physics 3 Tu-Th Section - hep.ucsb.eduhep.ucsb.edu/people/claudio/ph3-04/lecture1.pdf · unperturbed, stretched string x y. 12 Mathematical description (sinusoidal wave)

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Fall 2004 Physics 3Tu-Th Section

Claudio Campagnari

Web page: http://hep.ucsb.edu/people/claudio/ph3-04/

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Chapter 15: WavesWhat is a wave?

From www.dictionary.com:Physics.

– A disturbance traveling through a medium by which energy is transferred from one particle of the medium to another without causing any permanent displacement of the medium itself.

– A graphic representation of the variation of such a disturbance with time.

– A single cycle of such a disturbance.

Close, but not quite right!!!

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"disturbance" and "medium"

Disturbance = displacement from equilibrium

Medium = material in which displacement occurs

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Combined long. and transv. wave on liquid surface

ExamplesTransverse wave on a string

Longitudinal wave in a fluid (sound)

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So what's wrong with dictionary.com?

• There are waves that do not need a "medium" to propagate.

• e.g., Electromagnetic Waves (light) can propagate in vacuum.– This was a hard concept to swallow at the end

of the 19th century, but it is the way it is.• For now we concentrate on mechanical

waves that propagate in a medium.

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Longitudinal vs. Transverse

• Longitudinal: the disturbance is parallel to the direction of propagation.

• Transverse: the disturbance is perpendicularto the direction of propagation.

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Wave Velocity (Speed)The "disturbance" propagates in space

t = t0 t = to + ∆t

∆x

Do not confuse the velocity of the wave with the velocity of the particles in the medium

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Wave pulses vs. periodic waves

v

v

In a periodic wave the disturbance repeats itself and the motion of the particles of the medium is periodic

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Sinusoidal waves• Special case of periodic wave where the

motion of each particle in the medium is simple harmonic with the same amplitudeand the same frequency.

• Resulting wave is a symmetrical sequence of crests and troughs:

• Important because any periodic wave can be represented as the sum of sinusoidal waves (Fourier decomposition)

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Sinusoidal waves (cont.)Wavelength (λ):Distance over which displacement repeats

Period (T):Time over which displacement repeats

Frequency (f):f=1/T

Velocity (v):v = λ/T = λf

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Mathematical Description

• Waves on a string for concreteness

• Wave Function: a function that describes the position of any particle at any time:

• y(x,t)• Take y=0 as equilibrium position, i.e.,

unperturbed, stretched string

x

y

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Mathematical description (sinusoidal wave)• Take particle at x=0. Its motion is described by

y(x=0,t).• It undergoes Simple Harmonic Motion (SHM)

– y(x=0,t) = A cos(ωt+δ) = A cosωt (set δ=0)• What is then y(x,t), i.e., the displacement at any

other position along the string?• The disturbance travels with velocity v.• The motion at any x at a given time t is the same as

it was at x=0 at a time t-x/v

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Nothing fundamental here: just different ways of writing the same thing.........

Note: this is for waves moving in positive x-direction. For a wave moving in negativex-direction, kx-ωt becomes kx+ωt

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Aside: sines and cosines, don't get confused!

• SHM• y = A sin(ωt+δ)

= A cosδ sinωt + A sinδ cosωt• If you choose

– δ =0 y = A sinωt– δ = 90o y = A cosωt

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The wave equationFamiliar SHM properties:

But also:

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So:

Wave Equation:

One of the most important equations in physics.Whenever we encounter it we can say that adisturbance ("y") can propagate along the x-axis with velocity v.

Page 17: Fall 2004 Physics 3 Tu-Th Section - hep.ucsb.eduhep.ucsb.edu/people/claudio/ph3-04/lecture1.pdf · unperturbed, stretched string x y. 12 Mathematical description (sinusoidal wave)

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• Any function y(x,t)=y(x±vt) is a solution of the wave equation.

or

etc..........• All these functions represent disturbances

propagating to the right or the left with speed v

For example:

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Proof that y(x±vt) is solution of wave equation

So left-hand side of wave equation:

Let z = x ± vt so that y(x,t)=y(x±vt)=y(z)

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Right-hand side of wave equation:

Left-hand side was

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Wave equation for a string• F = string tension • µ = string mass/unit length = M/L• Ignore weight (gravity), ignore stretching of string• Look at forces on length ∆x of string

No horizontal motion,so x-components areequal and opposite

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Wave equation for string

• Derived with no assumption on shape• V2 = F/µ• Does it make intuitive sense?

– V increases with F (restoring force)– V decreases with mass (inertia)


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