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Wave Energy and Superposition Physics 202 Professor Lee Carkner Lecture 7
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Consider mark made on a piece of string with a wave traveling down it. At what point does the mark have the largest velocity? : At what point does the mark have the largest acceleration? a)In the middle : At the top b)At the top : In the middle c)In the middle : In the middle d)At the top: At the top e)Velocity and acceleration are constant
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Suppose you are producing a wave on a string by shaking. What properties of the wave do you directly control? a)Amplitude b)Wavelength c)Frequency d)Propagation velocity e)a and c only
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PAL #6 Waves =2 /k so A = , B = /2, C = /3 T = 2 / so T A = , T B = 1/3 , T C = 1/4 Which wave has largest transverse velocity? Wave C: largest amplitude, shortest period Largest wave speed? v = f = /T, v A = 1, v B = 1.5, v C = 1.3 A: y=2sin(2x-2t), B: y=4sin(4x-6t), C: y=6sin(6x-8t)
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PAL #6 Waves (cont.) Wave with y = 2 sin (2x-2t), find time when x= 5.2 cm has max a Happens when y = y m = 2 2 = 2 sin (2x-2t) 1 = sin (2x-2t) arcsin 1 = 2x-2t /2 = (2x - 2t) t = [2x-( /2)]/2 t = 4.4 seconds Maximum velocity when y = 0 0 = sin (2x-2t) 2x -2t = arcsin 0 = 0 t = x t = 5.2 seconds
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Velocity and the Medium If you send a pulse down a string what properties of the string will affect the wave motion? Tension ( ) If you force the string up, tension brings it back down Linear density ( = m/l =mass/length) You have to convert the PE to KE to have the string move
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Wave Tension in a String
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Force Balance on a String Element Consider a small piece of string l of linear density with a tension pulling on each end moving in a very small arc a distance R from rest There is a force balance between tension force: and centripetal force: Solving for v, This is also equal to our previous expression for v v = f
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String Properties How do we affect wave speed? v = ( ) ½ = f Wave speed is solely a property of the medium The wavelength then comes from the equation above The wavelength of a wave on a string depends on how fast you move it and the string properties
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Tension and Frequency
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Energy A wave on a string has both kinetic and elastic potential energy Every time we shake the string up and down we add a little more energy This energy is transmitted down the string The energy of a given piece of string changes with time as the string stretches and relaxes Assuming no energy dissipation
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Power Dependency P=½ v 2 y m 2 If we want to move a lot of energy fast, we want to add a lot of energy to the string and then have it move on a high velocity wave y m and depend on the wave generation process
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Superposition When 2 waves overlap each other they add algebraically Traveling waves only add up as they overlap and then continue on Waves can pass right through each other with no lasting effect
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Pulse Collision
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Interference The waves may be offset by a phase constant y 1 = y m sin (kx - t) y 2 = y m sin (kx - t + ) y r = y mr sin (kx - t +½ ) What is y mr (the resulting amplitude)? Is it greater or less than y m ?
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Interference and Phase y mr = 2 y m cos (½ ) The phase constant can be expressed in degrees, radians or wavelengths Example: 180 degrees = radians = 0.5 wavelengths
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Resultant Equation
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Combining Waves
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Types of Interference Constructive Interference -- when the resultant has a larger amplitude than the originals No offset or offset by a full wavelength Destructive Interference -- when the resultant has a smaller amplitude than the originals Offset by 1/2 wavelength
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Next Time Read: 16.11-16.13 Homework: Ch 16, P: 20, 30, 40, 83
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