Download presentation
Presentation is loading. Please wait.
Published byAnnabella Hall Modified over 9 years ago
1
MUSICAL ACOUSTICS Chapter 2 VIBRATING SYSTEMS
2
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.
3
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.
4
Vibratory motion: y,v, and a all change with time.
5
Displacement of a damped vibrator whose amplitude decreases with time
6
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:
7
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.
8
SIMPLE VIBRATING SYSTEMS A simple pendulum
9
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
10
SIMPLE VIBRATING SYSTEMS A piston free to vibrate in a cylinder
11
SIMPLE VIBRATING SYSTEMS A piston free to vibrate in a cylinder A Helmholtz resonator
12
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
13
SYSTEMS WITH TWO MASSES
14
Longitudinal vibrations of a three-mass vibrator Transverse vibration of a three-mass vibrator Transverse vibrations for spring systems with multiple masses
15
LINEAR ARRAY OF OSCILLATORS
16
MODES OF CIRCULAR MEMBRANES
17
BASS DRUM SNARE DRUM TIMPANI
18
VIBRATING BARS Both ends freeOne end clamped Arrows locate the nodes
19
CHLADNI PATTERNS OF A CIRCULAR PLATE SALT COLLECTS AT THE NODES
20
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
21
HOLOGRAPHIC INTERFEROMETRY
22
VIBRATIONAL MODES OF A CYMBAL (top) AND A CIRCULAR PLATE (bottom)
23
CYMBALS GONG TAM TAM
24
VIBRATIONS OF A TUNING FORK
25
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
26
ASSIGNMENT FOR MONDAY, Jan. 12 READ CHAPTER 3 EXERCISES IN CHAPTER 2: 1-7
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.