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Oscillations and Waves
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Pendulum Harmonic wave with only one frequency N W
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Mass on a spring Harmonic wave with only one frequency
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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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Mechanical Resonance Mechanical resonance is the tendency of a mechanicalsystem to respond at greater amplitude when the frequency of its oscillations matches the system's natural frequency of vibration (its resonance frequency or resonant frequency) than it does at other frequencies. The system responded as the frequency of its oscillations matched the natural frequency of vibration due to the wind.
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Resonance in a wave Resonance - The increase in amplitude of oscillation of an electric or mechanical system exposed to a periodic force whose frequency is equal or very close to the natural undamped frequency of the system.
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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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Confined waves Only waves with wavelengths that just fit in survive
(all others cancel themselves out)
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Harmonics For every given frequency, there are other frequencies that perfectly fit in the same space. These are called harmonics. They are whole divisions of the original wavelength, or multiples of the basic frequency. This is well known in musical instruments.
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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 = L/2; 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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Standing waves in a closed tube
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Standing waves in an open pipe
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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 higher)
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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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