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Acoustic Models
“It's easy to play any musical instrument: all you have to do is touch the right key
at the right time and the instrument will play itself,” J.S. Bach
Motivating Applications
Jet Noise Reduction:
• Employ chevrons to improve
mixing and decrease jet noise
• Boeing experiments demonstrate
4 dB noise reduction
• 3 dB reduction if 1 of 2 engines
turned off
• Influences aeroacoustic coupling
and requires 2-D and 3-D SMA
models
Reference: F.T. Calkins and J.H. Mabe,
“Variable geometry jet nozzle using
shape memory alloy actuators”
Motivating Applications
Duct Noise: Use secondary sources or
structure-borne actuators to reduce duct
or fan noise
Noise Canceling Headphones:
e.g., cockpit noise for pilots is a
significant problem for both
health and communication
Motivating Applications
Improved Instrument and Amplifier
Design: What makes a Stradivarius
unique?
Remote Acoustic Sensing: Can
we listen to a conversation
using a laser?
Motivating Applications
Seismology and Acoustic Medical
Imaging: e.g., ultrasound
Medical Treatment Strategies:
• Ultrasound to break up kidney stones
• Acoustic barriers for EM treatment
• Ultrasonic dental tools
Motivating Applications
Motivating Applications
SAW (Surface Acoustic Wave) Devices:
• Used in filters, oscillators and
transformers; e.g., bandpass filters in cell
phones
• Relies on transduction capabilities of PZT
Experimental image of SAW on
a crystal of tellurium oxide.
Basic Definitions
Acoustics: The science of sound including its production, transmission, and
effects.
Sound: A traveling wave created by a vibrating object and propagated through
a medium (gas, liquid, or solid) due to particle interactions.
• Because it is due to particle interactions, it is a mechanical wave. Thus sound
cannot travel through a vacuum --- “In space, no one can hear you scream,”
Alien 1979
• Particle interactions yield oscillations in pressure resulting in local regions of
compression and rarefaction.
Noise: Unwanted sound.
Sound Pressure and Acoustic Units
Acoustic or Sound Pressure: Difference between average local pressure of
medium and pressure within sound wave at same point and time.
• Think about difference between changing pressure in an airplane
(medium) and conversation (sound wave).
Instantaneous Sound Pressure:
RMS Sound Pressure:
Sound Pressure Levels
Sound Pressure Level: Employs logarithmic scale
Nondimensional Units: Decibels (dB)
Examples of Sound Pressure and Sound Pressure Levels
110-1406-200Jet engine at 100 m
100.00006Quiet rustling leaves
40-600.002-0.02Normal Talking
Approx 850.6Hearing damage (long
term exposure)
Approx 1002Jackhammer/Disco
Approx 12020Hearing damage (short
term exposure)
Approx 165Rocket launch
170-180Stun grenades
Approx 180 at 100 miles1883 Krakatoa eruption
191101,325Theoretical limit for
undistorted sound
dB re 20 microPAPa
Sound Pressure LevelRMS Sound PressureSound Source
Acoustic Sources
Direct Source:
Structural-Acoustic Coupling:
Aeroacoustic Coupling:
Note: Nature of sources affects
control strategies including choice
of actuators and sensors.
Physical Phenomena to be Modeled
Recall: Particle interactions yield oscillations in pressure resulting in local
regions of compression and rarefaction.
Mechanisms:
• Particles move: Conservation of mass
• Particles transmit energy (momentum):
Conservation of momentum
Conservation of Mass
Recall: (see Mass Conservation and Compartmental Analysis Notes)
1-D:
Continuity Equation
Fick’s law with transport
3-D: No diffusion
Conservation of Momentum: Lagrangian Description
Newton’s Second Law:
Note:
Conservation of Momentum
Euler’s Equation
Conservation of Momentum: Eulerian Description
3-D Eulerian Description: Consider stationary volume
Principle:
Conservation of Momentum: Eulerian Description
Momentum Balance: x-direction
Momentum: x-component
Momentum: y-component
Momentum: z-component
Conservation of Momentum
Note: Combination with the continuity equation yields
Euler’s Equations:
Equation of State
Conservation of Mass and Momentum:
Note: Need additional relation (constraint)
Barotropic Fluid: Pressure is a function only of density
Ideal Gas:
Models for Sound Waves
Nonlinear System:
Assumption: Sound is perturbations of pressure and density about static or
slowly time-varying state.
Static Quantities:
Models for Sound Waves
Dynamic Perturbations:
Strategy: Linearize about steady, silent case
Euler’s Equation: Momentum
Models for Sound Waves
Continuity Equation: Mass
Equation of State:
Wave Equation in Pressure
First-Order Equations for Sound:
Wave Equation in Pressure:
Wave Equation in Velocity
Wave Equation in Velocity: Note that
Additional Assumption:
Irrotational Flow:
Wave Equation in Potential
Initial Assumption:
Wave Equation in Potential
WLOG:
Wave Equation in Potential
Nonconstant Density:
Wave Equation in Potential: See book, pages 236-237
Linear Wave Equations for Sound
Pressure:
Velocity:
Potential:
Music
Pitch: This is simply the frequency of pure tones; e.g.,
Middle C is about 261.6 Hz as calculated in relation to
A above Middle C which as a frequency of 440 Hz.
Note: Going up an octave doubles the frequency. This is easily observed on
a guitar where pressing at the twelfth fret cuts the string in half which
doubles the frequency and raises the tone an octave.
Music
Note: Going up a fifth (e.g., C and G) causes frequencies to align every third
interval for the G --- e.g., First two notes of Star Wars theme.
Reason: Equal tempering which spaces all 12 notes equally
• Each semitone is thus
• C sharp thus has a frequency of
• G has a frequency of
• A:
Music
Note: Include a 3rd (E) and a fifth (G) -- C major chord
Note: Raising the key causes the confluence to occur more quickly.
Music
Note: The wavelengths of notes is related to their frequency by the expression
where c = 343 m/s for air.
Example: The wavelength of Middle C is thus 1.31 m.

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Acoustic wave form

  • 1. Acoustic Models “It's easy to play any musical instrument: all you have to do is touch the right key at the right time and the instrument will play itself,” J.S. Bach
  • 2. Motivating Applications Jet Noise Reduction: • Employ chevrons to improve mixing and decrease jet noise • Boeing experiments demonstrate 4 dB noise reduction • 3 dB reduction if 1 of 2 engines turned off • Influences aeroacoustic coupling and requires 2-D and 3-D SMA models Reference: F.T. Calkins and J.H. Mabe, “Variable geometry jet nozzle using shape memory alloy actuators”
  • 3. Motivating Applications Duct Noise: Use secondary sources or structure-borne actuators to reduce duct or fan noise Noise Canceling Headphones: e.g., cockpit noise for pilots is a significant problem for both health and communication
  • 4. Motivating Applications Improved Instrument and Amplifier Design: What makes a Stradivarius unique? Remote Acoustic Sensing: Can we listen to a conversation using a laser?
  • 5. Motivating Applications Seismology and Acoustic Medical Imaging: e.g., ultrasound
  • 6. Medical Treatment Strategies: • Ultrasound to break up kidney stones • Acoustic barriers for EM treatment • Ultrasonic dental tools Motivating Applications
  • 7. Motivating Applications SAW (Surface Acoustic Wave) Devices: • Used in filters, oscillators and transformers; e.g., bandpass filters in cell phones • Relies on transduction capabilities of PZT Experimental image of SAW on a crystal of tellurium oxide.
  • 8. Basic Definitions Acoustics: The science of sound including its production, transmission, and effects. Sound: A traveling wave created by a vibrating object and propagated through a medium (gas, liquid, or solid) due to particle interactions. • Because it is due to particle interactions, it is a mechanical wave. Thus sound cannot travel through a vacuum --- “In space, no one can hear you scream,” Alien 1979 • Particle interactions yield oscillations in pressure resulting in local regions of compression and rarefaction. Noise: Unwanted sound.
  • 9. Sound Pressure and Acoustic Units Acoustic or Sound Pressure: Difference between average local pressure of medium and pressure within sound wave at same point and time. • Think about difference between changing pressure in an airplane (medium) and conversation (sound wave). Instantaneous Sound Pressure: RMS Sound Pressure:
  • 10. Sound Pressure Levels Sound Pressure Level: Employs logarithmic scale Nondimensional Units: Decibels (dB)
  • 11. Examples of Sound Pressure and Sound Pressure Levels 110-1406-200Jet engine at 100 m 100.00006Quiet rustling leaves 40-600.002-0.02Normal Talking Approx 850.6Hearing damage (long term exposure) Approx 1002Jackhammer/Disco Approx 12020Hearing damage (short term exposure) Approx 165Rocket launch 170-180Stun grenades Approx 180 at 100 miles1883 Krakatoa eruption 191101,325Theoretical limit for undistorted sound dB re 20 microPAPa Sound Pressure LevelRMS Sound PressureSound Source
  • 12. Acoustic Sources Direct Source: Structural-Acoustic Coupling: Aeroacoustic Coupling: Note: Nature of sources affects control strategies including choice of actuators and sensors.
  • 13. Physical Phenomena to be Modeled Recall: Particle interactions yield oscillations in pressure resulting in local regions of compression and rarefaction. Mechanisms: • Particles move: Conservation of mass • Particles transmit energy (momentum): Conservation of momentum
  • 14. Conservation of Mass Recall: (see Mass Conservation and Compartmental Analysis Notes) 1-D: Continuity Equation Fick’s law with transport 3-D: No diffusion
  • 15. Conservation of Momentum: Lagrangian Description Newton’s Second Law: Note:
  • 17. Conservation of Momentum: Eulerian Description 3-D Eulerian Description: Consider stationary volume Principle:
  • 18. Conservation of Momentum: Eulerian Description Momentum Balance: x-direction Momentum: x-component Momentum: y-component Momentum: z-component
  • 19. Conservation of Momentum Note: Combination with the continuity equation yields Euler’s Equations:
  • 20. Equation of State Conservation of Mass and Momentum: Note: Need additional relation (constraint) Barotropic Fluid: Pressure is a function only of density Ideal Gas:
  • 21. Models for Sound Waves Nonlinear System: Assumption: Sound is perturbations of pressure and density about static or slowly time-varying state. Static Quantities:
  • 22. Models for Sound Waves Dynamic Perturbations: Strategy: Linearize about steady, silent case Euler’s Equation: Momentum
  • 23. Models for Sound Waves Continuity Equation: Mass Equation of State:
  • 24. Wave Equation in Pressure First-Order Equations for Sound: Wave Equation in Pressure:
  • 25. Wave Equation in Velocity Wave Equation in Velocity: Note that Additional Assumption: Irrotational Flow:
  • 26. Wave Equation in Potential Initial Assumption:
  • 27. Wave Equation in Potential WLOG:
  • 28. Wave Equation in Potential Nonconstant Density: Wave Equation in Potential: See book, pages 236-237
  • 29. Linear Wave Equations for Sound Pressure: Velocity: Potential:
  • 30. Music Pitch: This is simply the frequency of pure tones; e.g., Middle C is about 261.6 Hz as calculated in relation to A above Middle C which as a frequency of 440 Hz. Note: Going up an octave doubles the frequency. This is easily observed on a guitar where pressing at the twelfth fret cuts the string in half which doubles the frequency and raises the tone an octave.
  • 31. Music Note: Going up a fifth (e.g., C and G) causes frequencies to align every third interval for the G --- e.g., First two notes of Star Wars theme. Reason: Equal tempering which spaces all 12 notes equally • Each semitone is thus • C sharp thus has a frequency of • G has a frequency of • A:
  • 32. Music Note: Include a 3rd (E) and a fifth (G) -- C major chord Note: Raising the key causes the confluence to occur more quickly.
  • 33. Music Note: The wavelengths of notes is related to their frequency by the expression where c = 343 m/s for air. Example: The wavelength of Middle C is thus 1.31 m.