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MUSICAL ACOUSTICS Chapter 2 VIBRATING SYSTEMS
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SIMPLE HARMONIC MOTION A simple vibrator consisting of a mass and a spring. At equilibrium (center), the upward force exerted by the spring and the force of gravity balance each other, and the net force F on the mass is zero.
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Simple Harmonic Motion Graphs of simple harmonic motion: (a) Displacement versus time (b) Speed versus Time. Note that speed reaches its maximum when displacement is zero and vice versa.
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Vibratory motion: y,v, and a all change with time.
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Displacement of a damped vibrator whose amplitude decreases with time
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Representing a Vibrating System Waveform Spectrum
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EVERY VIBRATING SYSTEM HAS Inertia (mass) Elasticity (spring) For a mass/spring Hooke’s Law F = Ky In Chapter 1 we learned that KE= ½ mv 2 Similarly, it can be shown that PE = ½ Ky 2 If the vibrator has damping:
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A mass hangs from a spring. You raise the mass 1 cm, hold it there for a short time and then let it drop Make a graph of its motion Make a graph of its total energy.
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SIMPLE VIBRATING SYSTEMS A simple pendulum
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A mass-spring system vibrates at a frequency f If the mass is doubled: a)The frequency will be 2 f b)The frequency will be √2 f c)The frequency will remain f d)The frequency will be f /√2 e) The frequency will be f /2
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A mass-spring system vibrates at a frequency f If the mass is doubled: a)The frequency will be 2 f b)The frequency will be √2 f c)The frequency will remain f d)The frequency will be f /√2 e) The frequency will be f /2 A mass swings on the end of a string at frequency f If the mass is doubled: a)The frequency will be 2 f b) The frequency will be √2 f c)The frequency will remain f d)The frequency will be f /√2 e) The frequency will be f/ 2
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SIMPLE VIBRATING SYSTEMS A piston free to vibrate in a cylinder
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SIMPLE VIBRATING SYSTEMS A piston free to vibrate in a cylinder A Helmholtz resonator
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SIMPLE VIBRATING SYSTEMS A piston free to vibrate in a cylinder A Helmholtz resonator m= ρ ɑ l K=ρ ɑ 2 l 2 /V
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SYSTEMS WITH TWO MASSES
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Longitudinal vibrations of a three-mass vibrator Transverse vibration of a three-mass vibrator Transverse vibrations for spring systems with multiple masses
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LINEAR ARRAY OF OSCILLATORS
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MODES OF CIRCULAR MEMBRANES
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BASS DRUM SNARE DRUM TIMPANI
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VIBRATING BARS Both ends freeOne end clamped Arrows locate the nodes
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CHLADNI PATTERNS OF A CIRCULAR PLATE SALT COLLECTS AT THE NODES
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CHLADNI PATTERNS JOE WOLFE’S PHYSCLIPS ON MODES OF VIBRATION AND CHLADNI PATTERN CAN BE ACCESSED AT p://www.phys.unsw.edu.au/jw/chladni.html#modes http://www.phys.unsw.edu.au/jw/chladni.html#modes p://www.phys.unsw.edu.au/jw/chladni.html#modes
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HOLOGRAPHIC INTERFEROMETRY
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VIBRATIONAL MODES OF A CYMBAL (top) AND A CIRCULAR PLATE (bottom)
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CYMBALS GONG TAM TAM
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VIBRATIONS OF A TUNING FORK
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ANIMATIONS OF TUNING FORK VIBRATIONS AT DAN RUSSELL’S WEBSITE http//www.acs.psu.edu/drussell/Demos/TuningFork/fork- modes.html http://www.acs.psu.edu/drussell/Demos/TuningFork/fork- mohttp://www.acs.psu.edu/drussell/Demos/TuningFork/fork-modes.html des.html http://www.acs.psu.edu/drussell/Demos/TuningFork/fork- mohttp://www.acs.psu.edu/drussell/Demos/TuningFork/fork-modes.html des.html HTT ttp://www.acs.psu.edu/drussell/De mos/TuningFork/fork-modes.html http://www.acs.psu.edu/drussehttp:// www.acs.psu.edu/drussell/Demos/Tu ningFork/fork-modes.html ll/Demos/TuningFork/fork- modes.hthhttp://www.acs.psu.edu/dru ssell/Demos/TuningFork/fork- mohttp://www.acs.psu.edu/drussell/D emos/TuningFork/fork-modes.html des.html http://www.acs.psu.edu/drussell/Dem os/TuningFork/fork-modes.html ttp://www.acs.psu.edu/drussell/Demo s/TuningFork/fork-modes.html
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Vibration spectrum of a plucked string A Spectrum is a graph of Amplitude vs Frequency
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ASSIGNMENT FOR MONDAY, Jan. 11 READ CHAPTER 3 EXERCISES IN CHAPTER 2: 1-7
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