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P105 Lecture #27 visuals 20 March 2013
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Sound production from vocal system
Three components: Power source (lungs) Oscillator (vocal folds spring-mass system, driven by Bernoulli effect) Resonator / Radiator (vocal tract and mouth subject of today’s lecture) Recall, periodic emission of puffs of air though glottal opening (due to vibration of vocal folds), constitutes a pressure wave with a discrete (harmonic) frequency spectrum: fundamental is at the vocal fold vibration frequency & determines the pitch; harmonics are down by 12 dB after each octave (factor of 2 increase in frequency). i.e., LI (n=2) = LI (n=1) – 12 dB; LI (n=4) = LI (n=2) – 12 dB, etc. To understand harmonic structure of speech & singing must also take into account the filtering effect of the vocal tract and mouth. This is the subject of today’s lecture.
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Net Result: Periodic expulsion of “puffs” of air from lungs
Top: volume velocity vs time for sound production at 125 Hz (male voice); Bottom: Power spectrum falls at 12 dB per octave Fourier Spectrum: From Rossing, Wheeler & Moore, The Science of Sound
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Impact of the vocal tract geometry:
Formants Can think of the vocal tract as an air-filled pipe, closed at one end (folds) & open at the other (mouth) Standing wave modes = “formants” Nominally odd harmonics only: fn = n (v / 4L), v = 343 m/s L ~ 17.5cm f1 ~ 500 Hz. In practice, geometry is complex, formant frequencies influenced by tongue, jaw mouth, etc… Illustration from J. Sundberg, “The Acoustics of the Singing Voice”
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How can you vary your formants?
Shape of oral cavity, mouth opening, & location of tongue are very important For example, a constriction at a location of a formant’s pressure node will limit impact of that formant Also, can amplify higher freq. modes with antinode at that location from J. Sundberg, “The Acoustics of the Singing Voice”
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Making different vowel sounds
from J. Sundberg, “The Acoustics of the Singing Voice”
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Making different vowel sounds
from J. Sundberg, “The Acoustics of the Singing Voice”
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