Thomas M. Huber, Brian Collins

Slides:



Advertisements
Similar presentations
Chapter 12 Parts of waves (review) Octaves Stringed Harmonics
Advertisements

Closed end: displacement zero (node), pressure max (antinode)
ISNS Phenomena of Nature Intensity decreases with increasing distance from the source. the wave is spreading out over a circular (2 dimensions)
Waves_03 1 Two sine waves travelling in opposite directions  standing wave Some animations courtesy of Dr. Dan Russell, Kettering University TRANSVERSE.
Harmonic Series and Spectrograms 220 Hz (A3) Why do they sound different? Instrument 1 Instrument 2Sine Wave.
Musical Instruments 1 Musical Instruments. Musical Instruments 2 Introductory Question Sound can break glass. Which is most likely to break: Sound can.
Musical Instruments 1 Musical Instruments. Musical Instruments 2 Introductory Question Sound can break glass. Which is most likely to break: Sound can.
Physics of Sounds Overview Properties of vibrating systems Free and forced vibrations Resonance and frequency response Sound waves in air Frequency, wavelength,
Chapter 14 Sound AP Physics B Lecture Notes.
9.2 Musical Instruments. New Ideas for today Sound and waves Pitch String and wind instruments.
Resonance and Sound Decay: A Quantitative Study of Acoustic guitars Acoustical Society of America Meeting October 3, 2005 by Erika Galazen and Joni Nordberg.
PH 105 Dr. Cecilia Vogel Lecture 19. OUTLINE  Woodwinds  single reed, double reed, air reed  bores: cylinder, cone  resonances, harmonics  register.
Principle of Superposition Interference Stationary Waves
PH 105 Dr. Cecilia Vogel Lecture 6. OUTLINE  Natural or Normal Modes  Driving force  Resonance  Helmholtz resonator  Standing Waves  Strings and.
7/5/20141FCI. Prof. Nabila M. Hassan Faculty of Computer and Information Fayoum University 2013/2014 7/5/20142FCI.
Harmonics and Overtones Waveforms / Wave Interaction Phase Concepts / Comb Filtering Beat Frequencies / Noise AUD202 Audio and Acoustics Theory.
1 If we try to produce a traveling harmonic wave on a rope, repeated reflections from the end produces a wave traveling in the opposite direction - with.
Noncontact modal testing of hard-drive suspensions using ultrasound radiation force Acoustical Society of America Meeting: October 18, 2005 Thomas M. Huber.
Selective modal excitation using phase- shifted ultrasound radiation force Acoustical Society of America Meeting June 2006 Thomas M. Huber Physics Department,
Waves and Sound Ch
Barry Latham Physics: Principles & Problems Glencoe Science, 2005.
Violins and Pipe Organs 1 Violins and Pipe Organs.
L 22 – Vibrations and Waves [3] resonance  clocks – pendulum  springs  harmonic motion  mechanical waves  sound waves  golden rule for waves Wave.
Harmonic Series and Spectrograms
MECHANICAL WAVES WAVE PROPERTIES SOUND…“WHAT?”
Musical Instruments Chapter 9 part C. Observations about Musical Instruments They can produce different notes They can produce different notes They.
Calculate the speed of 25 cm ripples passing through water at 120 waves/s.
Chapter 13 - Sound 13.1 Sound Waves.
Excitation of Vibrational Eigenstates of Coupled Microcantilevers Using Ultrasound Radiation Force ASME 2nd International Conference on Micro and Nanosystems.
Resonance Chapter 4. Concert Talk Resonance: definition When a vibrating system is driven by a force at a frequency near the natural frequency of the.
Chapter 15 Sounds.
Chapter 14 Sound. Sound waves Sound – longitudinal waves in a substance (air, water, metal, etc.) with frequencies detectable by human ears (between ~
Sound Sound waves are –Longitudinal –Pressure Waves Infrasonic – less than 20 Hz Audible – between 20 and 20,000 Hz Ultrasonic – greater than 20,000 Hz.
Ch. 15 Sound Milbank High School. Sec Properties of Sound Objectives –Demonstrate knowledge of the nature of sound waves and the properties sound.
Noncontact Modal Analysis of a Pipe Organ Reed using Airborne Ultrasound Stimulated Vibrometry May 25, 2004 Acoustical Society of America Meeting Thomas.
L 23 – Vibrations and Waves [3]  resonance   clocks – pendulum   springs   harmonic motion   mechanical waves   sound waves  golden rule for.
Tuning Fork Scanning Probe Microscopy Mesoscopic Group Meeting November 29, 2007.
 Depends on relative motion of source and detector  Closer = decr wavelength › Incr pitch › Blue shift  Farther = incr wavelength › Decr pitch › Red.
Harmonic Series and Spectrograms BY JORDAN KEARNS (W&L ‘14) & JON ERICKSON (STILL HERE )
Noncontact Modal Excitation of Small Structures Using Ultrasound Radiation Force Society for Experimental Mechanics Annual Meeting Springfield, MA June.
Wave Interference Superposition Principle – when two or more waves encounter each other while traveling through a medium, the resultant wave is found by.
The Physics of Music Waves
L 22 – Vibrations and Waves [3]
Closed Pipe Pipe closed at ONE end: closed end pressure antinode air press. L = /4 L.
Chapter 12 Sound Producing a Sound Wave Characteristics of Sound Waves The Speed of Sound Spherical and Plane Waves The.
L 23 – Vibrations and Waves [3]  resonance   clocks – pendulum   springs   harmonic motion   mechanical waves   sound waves  golden rule for.
Non-contact mode excitation of small structures in air using ultrasound radiation force Acoustical Society of America Meeting: May 17, 2005 Thomas M. Huber,
1 L 23 – Vibrations and Waves [3]  resonance  clocks – pendulum  springs  harmonic motion  mechanical waves  sound waves  golden rule for waves.
Resonant Waves in A Vibrating Column of Air For a tube open at both ends:
Harmonics. Strings as Harmonic Oscillators Its mass gives it inertia Its mass gives it inertia Its tension and curvature give it a restoring force Its.
Physics Section 12.3 Apply the properties of sound resonance Recall: A standing wave is the result of the superposition of a wave and its reflection from.
15.1 Properties and Detection of Sound Interference of sound waves.
1 Chapter 15 Objectives: 1) Explain a sound wave in terms of wave type and classification. 2) Describe a medium’s characteristics that affect the speed.
Holt Physics Chapter 12 Waves Periodic Motion A repeated motion that is back and forth over the same path.
Intro to Fourier Series BY JORDAN KEARNS (W&L ‘14) & JON ERICKSON (STILL HERE )
SPM Users Basic Training August 2010 Lecture VIII – AC Imaging Modes: ACAFM and MAC Imaging methods using oscillating cantilevers.
Physics 1 What is a wave? A wave is: an energy-transferring disturbance moves through a material medium or a vacuum.
Waves 1 The Transfer of Energy. The Basics: A λ d(m) (#λ or m) d = displacement Amplitude = max displacement from origin λ = wavelength (in m) f = frequency.
Imaging of propagating wave fronts resulting from ultrasonic pulses incident on heel bones using refracto-vibrometry Acoustical Society of America Meeting.
Chapter Summary 15.1 Properties and Detection of Sound
L 22 – Vibrations and Waves [3]
Principle of Superposition Interference Stationary Waves
Examples of wave superposition
Waves 1 The Transfer of Energy.
Standing Waves Resonance.
Example Which type of wave requires a material medium to travel through? a) Television b) Light c) Sound d) Radio e) X-ray Sound is a mechanical wave,
Lecture 7 Ch 16 Standing waves
Mechanical Waves © 2014 Pearson Education, Inc..
Closed end: displacement zero (node), pressure max (antinode)
Sound Chapter 12.
Presentation transcript:

Thomas M. Huber, Brian Collins Scanning Vibrometer Studies of Organ Pipes Presentation for November 2003 Acoustical Society of America Meeting Thomas M. Huber, Brian Collins Physics Department, Gustavus Adolphus College Charles Hendrickson Hendrickson Organ Company Mario Pineda Polytec PI, Incorporated

Overview Organ reed pipes Previous laser vibrometer studies of reed pipes Scanning vibrometer measurements of air-driven reed Scanning vibrometer measurements of mechanically driven reed Conclusions

Organ Reed Pipe Thin brass reed firmly clamped at one end by the wedge Tuning wire holds reed against the stationary shallot Moving the tuning wire adjusts pitch Pitch is determined almost entirely by the length of vibrating reed The resonator plays a secondary role in selecting the pitch

Research in Reed Organ Pipe Acoustics Research since 1940’s primarily with microphones & spectral analysis Measured audio spectra have integer-multiple harmonics Integer-multiple harmonics not due to resonator (since they are present regardless of the pitch selected by adjusting the tuning wire)

Laser Vibrometer Studies of Reed Pipes Since mid 1990’s: Tom Rossing & others use laser vibrometer on reed Laser emitted from vibrometer head Reflects off small spot on vibrating reed surface Doppler shift of light allows Determination of velocity of the reed surface at a point Displacement of the reed surface from equilibrium

Results of Previous Vibrometer Studies Integer-multiple harmonics not due to resonator (since they are present regardless of the pitch selected by adjusting the tuning wire) Because the reed strikes the shallot, there is an asymmetry in its motion (similar to a rectified sine wave) Prevailing Hypothesis: Integer-Multiple harmonics due to the mechanical interaction between reed and shallot

Our Experiment Goals Better understanding of origin of integer-multiple harmonics Measure the vibrational deflection shapes of the reed To understand the modes, study mechanically driven reed In vacuum and atmospheric pressure Use a Polytec PSV-300 scanning vibrometer Available for 5 days at Gustavus Adolphus College

Polytec PSV-300 Scanning Vibrometer Scanning vibrometer uses optical system to deflect beam across vibrating surface Measures both amplitude and phase at each point Highlight section of spectrum and software plots 3-D deflection shape Rotated Image Showing Displacement Face-On View Of Vibrating Reed Scan Points Measured on Surface

Results from Air-Driven Pipe Most harmonics have complicated deflection shapes Modes exist where entire reed and tuning wire are in motion 8th Harmonic 3rd Order ENTIRE REED 6.52 kHz 1st Harmonic Simple Cantilever 813 Hz 4th Harmonic Torsional 3.26 kHz 5th Harmonic 2nd Order Cantilever 4.08 kHz

Mechanically Driven Reed Pipe Use a mechanical oscillator to drive the reed Chirp sine wave applied by mechanical driver to back of shallot Large amplitude vibration when at resonant frequency of reed This technique Can be driven in vacuum or atmospheric pressure to isolate reed-air couplings Allows control over amplitude of vibration

Results for Mechanically Driven Pipe in Vacuum Cantilever modes occur at frequencies consistent with theory Also observed are integer-multiple harmonics of fundamental. These are due to expected mechanical interaction between reed and shallot Simple Cantilever Measured: 0.72 kHz Theory: 0.70 kHz Torsional Measured: 2.47 kHz Theory: 2.9 kHz 2nd Cantilever Measured: 4.54 kHz Theory: 4.4 kHz 3rd Cantilever Entire Measured: 6.5 kHz Theory: 6.1 kHz

Mechanical Driving: Comparison of Vacuum and Atmospheric Pressure When driven with same amplitude in air, two effects occur Increase in the integer multiple harmonics of fundamental Decrease in the “natural” modes of the cantilever Indicates that air-reed interaction plays a role in origin of integer-multiple harmonics. Not just reed-shallot interactions

http://physics.gustavus.edu/~huber/organs Conclusions Polytec scanning vibrometer provides an entirely new view of vibrational modes of this system Vibration of blown reed includes torsional and higher-order cantilever modes; these are acoustically important Modes with significant displacement of entire reed and tuning wire are also present in blown reed Modes of mechanically driven reed in vacuum agree with theoretically predicted frequencies Air-reed interactions play a role in producing integer-multiple harmonics; not just mechanical reed-shallot interaction http://physics.gustavus.edu/~huber/organs