the song of glasses lain - umr cnrs 5011 univ. montpellier 2 - cc 82 34095 montpellier cedex 5...

21
THE SONG OF GLASSES THE SONG OF GLASSES LAIN - UMR CNRS 5011 Univ. Montpellier 2 - cc 82 34095 MONTPELLIER cedex 5 FRANCE Ing. Jean-Yves Ferrandis Pr. Gerard Leveque Pr. Jacques Attal

Upload: coleen-pitts

Post on 24-Dec-2015

216 views

Category:

Documents


1 download

TRANSCRIPT

  • Slide 1
  • THE SONG OF GLASSES LAIN - UMR CNRS 5011 Univ. Montpellier 2 - cc 82 34095 MONTPELLIER cedex 5 FRANCE Ing. Jean-Yves Ferrandis Pr. Gerard Leveque Pr. Jacques Attal
  • Slide 2
  • GOAL: STUDY OF THE HARMONY OF GLASSES n GOAL: STUDY OF THE HARMONY OF GLASSES Acoustical criteria the strike note : pitch and sound decay timbre consonance and dissonance Subjective approach
  • Slide 3
  • n I. Sound analysis : theoretical background n II. Experiences on glasses and crystal glasses n III. Discussion n IV. Test of listening n V. Conclusions FRAME WORK
  • Slide 4
  • n Harmonic partials : string instruments n Inharmonic partials : infinite cylindrical pipes n Spectral analysis n Circular plates n Vibration of bells n Consonance intervals I. Sound analysis : theoreticalbackgrond
  • Slide 5
  • Harmonic partials : string instruments n String equation Solutions density S cross-area T strain force n order of the mode frequency n = 1, 2, 3, 4 . z TTx
  • Slide 6
  • Inharmonic partials : infinite cylindrical pipes n Infinite cylindrical pipes z : axis of the pipe : angle in the shear cut e : thickness of the pipe e, : Young modulus, Poisson coefficient R : radius of the pipe : density The partial mode are not harmonic frequency intervals [1, 8/3, 5, 8, 35/3 ]
  • Slide 7
  • 1234567 8 Cylinders Fondamental frequency m=2m=3 m = 1 m = 2 Spectral analysis m=4m=5 String vibrations 8/3
  • Slide 8
  • Circular plates Chladni s law (empirical relation ship) where c is the sound velocity (n,m) is the mode numbers for flat plates p = 2 for non flat plates (cymbals, bells) p < 2
  • Slide 9
  • Vibration of bells n The bells can be tuned on harmonic partials
  • Slide 10
  • Consonance intervals for bells
  • Slide 11
  • n Pitch n Sound decay n Warble II. Experiences on glasses and crystal glasses
  • Slide 12
  • Sound analysis : Typical response
  • Slide 13
  • : Time constant for a decay 0.368 Sound decay
  • Slide 14
  • Beats due to a dissimetry of the sample B A B A B A BWarble Tea cup
  • Slide 15
  • n Shape n Materials n Manufacturing III. Discussion : Effects of
  • Slide 16
  • Shape dependance The thicker the glass the higher the pitch f 2 /f 1 = 2.35 (tenth = 2.4 ) can be adjusted from 2 to 2.5 according to ellipticity f 2 /f 1 = 1.48f 3 /f 1 = 2.01 (quint = 1.5) can be adjusted with the opening angle ELLIPTICAL CONICAL
  • Slide 17
  • Materials dependance The time constant of the decay is four times as large for the crystal glass with same shape. The pitch and the timbre are correctly appreciated when the decay is small. Verre blancCristal
  • Slide 18
  • Spreading of the measurements (fundamental and first harmonic) Repeatability on a serial of identical glasses Manufacturing
  • Slide 19
  • Test procedure n Collect opinion from an audience of 25 people n Listening to synthetic sounds which simulates glass strikes : effect of pitch, timbre, time decay... u Note : This test has been performed on non informed audience, but is dependant on the musical background of each one IV. Test of listeing
  • Slide 20
  • V. Test and results Q : PITCH EFFECT : thickness and shapeA1B1 A : Preference for bass tones Q : TIME DECAYA2B2 A : Large agreement for long decay : crystal glass is unanimously appreciated Q : RATIO f 2 /f 1 A4B4B5B6 A : Audience can make difference between consonance and dissonance but does not agree on the appreciation Q : NUMBER OF PARTIALSA7B7 A : Slight preference for few partials
  • Slide 21
  • F PSYCHOLOGICAL IMPACT OF THE SONG OF THE GLASS PITCH TIMBRE TIME DECAY F MANUFACTURING QUALITY CONTROL F NEW DESIGN OF GLASS CONSONANT SERIALS NEW SHAPES WHICH ENHANCE SPECIFIC MODES Conclusions