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Oscillations and Waves
Micro-world Macro-world Lect 5
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Equilibrium (Fnet = 0)
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Examples of unstable Equilibrium
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Examples of Stable equilibrium
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Destabilizing forces N Fnet = 0 W
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Destabilizing forces N Fnet = away from equil W
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Destabilizing forces Fnet = away from equil N W
destabilizing forces always push the system further away from equilibrium
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restoring forces N Fnet = 0 W
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restoring forces N Fnet = toward equil. W
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restoring forces N Fnet = toward equil. W Restoring forces always push
the system back toward equilibrium
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Pendulum N W
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Mass on a spring
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Displacement vs time Displaced systems oscillate
around stable equil. points amplitude Equil. point period (=T)
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Simple harmonic motion
Pure Sine-like curve T Equil. point T= period = time for 1 complete oscillation = 1/T f = frequency = # of oscillations/time
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Masses on springs Animations courtesy of Dr. Dan Russell, Kettering University
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Not all oscillations are nice Sine curves
Equil. point T f=1/T
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Natural frequency f= (1/2p)k/m f= (1/2p)g/l
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Driven oscillators natural freq. = f0 f = 0.4f0 f = 1.1f0 f = 1.6f0
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Resonance (f=f0)
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Waves Animations courtesy of Dr. Dan Russell, Kettering University
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Wave in a string Animations courtesy of Dr. Dan Russell, Kettering University
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Pulsed Sound Wave
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Harmonic sound wave
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Harmonic sound wave
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V=fl or f=V/ l Harmonic wave =v =l l T = = fl = but 1/T=f distance
Wave speed =v Shake end of string up & down with SHM period = T wavelength =l l T distance time wavelength period Wave speed = v = = = fl = V=fl or f=V/ l but 1/T=f
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Reflection (from a fixed end)
Animations courtesy of Dr. Dan Russell, Kettering University
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Reflection (from a loose end)
Animations courtesy of Dr. Dan Russell, Kettering University
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Adding waves pulsed waves
Animations courtesy of Dr. Dan Russell, Kettering University
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Two waves in same direction with slightly different frequencies
Adding waves Two waves in same direction with slightly different frequencies Wave 1 Wave 2 resultant wave “Beats” Animations courtesy of Dr. Dan Russell, Kettering University
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Adding waves harmonic waves in opposite directions incident wave
reflected wave resultant wave (standing wave) Animations courtesy of Dr. Dan Russell, Kettering University
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Two wave sources constructive interference destructive interference
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Confined waves Only waves with wavelengths that just fit in survive
(all others cancel themselves out)
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Confined waves
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Allowed frequencies l= 2L f0=V/l = V/2L f1=V/l = V/L=2f0 l=L l=(2/3)L
Fundamental tone f1=V/l = V/L=2f0 l=L 1st overtone l=(2/3)L f2=V/l=V/(2/3)L=3f0 2nd overtone l=L/2 f3=V/l=V/(1/2)L=4f0 3rd overtone l=(2/5)L f4=V/l=V/(2/5)L=5f0 4th overtone
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Ukuleles, etc l0 = 2L; f0 = V/2L l1= L; f1 = V/L =2f0
l2= 2L/3; f2 = 3f0 L l3= L/2; f3 = 4f0 Etc… (V depends on the Tension & thickness Of the string)
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Vocal Range – Fundamental Pitch
♩ ♩ 1175 Hz ♩ 880 Hz ♩ 587 Hz ♩ 523 Hz ♩ 392 Hz 329 Hz 196 Hz 165 Hz 147 Hz 131 Hz 98 Hz 82 Hz Tenor C2 – C5 SopranoG3 – D6 ♂: ♀: Mezzo-SopranoE3 – A5 Baritone G2 – G4 Bass E2 – E4 ContraltoD3 – D5 Thanks to Kristine Ayson
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Doppler effect
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Sound wave stationary source
Wavelength same in all directions
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Sound wave moving source
Wavelength in forward direction is shorter (frequency is higher) Wavelength in backward direction is longer (frequency is lower)
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Waves from a stationary source
Wavelength same in all directions
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Waves from a moving source
Wavelength in backward direction is longer (frequency is higher) Wavelength in forward direction is shorter (frequency is higher)
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Visible light Short wavelengths Long wavelengths
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receding source red-shifted
approaching source blue-shifted
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Edwin Hubble
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More distant galaxies have bigger red shifts
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The universe is expanding!!
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Use red- & blue-shifts to study orbital motion of stars in galaxies
receding red-shifted approaching blue-shifted
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A typical galactic rotation curve
NGC 6503
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Large planets create red-shifts and blue shifts in the light of their star
Use this to detect planets & measure their orbital frequency
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Planetary motion induced stellar velocity
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