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CS 551/651: Structure of Spoken Language Lecture 3: Phonetic Symbols and Physiology of Speech Production John-Paul Hosom

CS 551/651: Structure of Spoken Language Lecture 3: Phonetic Symbols and Physiology of Speech Production John-Paul Hosom Fall 2008. More Formant Data…. (source unknown). Effects of Coarticulation. Phonetic Symbols: the IPA The International Phonetic Alphabet (IPA)

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CS 551/651: Structure of Spoken Language Lecture 3: Phonetic Symbols and Physiology of Speech Production John-Paul Hosom

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  1. CS 551/651: Structure of Spoken Language Lecture 3: Phonetic Symbols andPhysiology of Speech Production John-Paul Hosom Fall 2008

  2. More Formant Data… (source unknown)

  3. Effects of Coarticulation

  4. Phonetic Symbols: the IPA The International Phonetic Alphabet (IPA) (reproduced compliments of the International Phonetic Association, Department of Linguistics, University of Victoria, Victoria, British Columbia, Canada)

  5. Phonetic Symbols: the IPA

  6. Phonetic Symbols: the IPA Produced With tip of tongue, e.g. Spanish /r/ Tongue tip or blade touching upper lip

  7. Phonetic Symbols: the IPA Other IPA symbols…

  8. Phonetic Symbols: the IPA Examples:

  9. Phonetic Symbols: Worldbet An ASCII representation of IPA, developed by Hieronymous (AT&T)

  10. Phonetic Symbols: ARPAbet, TIMITbet, OGIbet ASCII representation of English used in TIMIT corpus.

  11. Phonetic Symbols: SAMPA An ASCII representation for multiple (European) languages

  12. Acoustic Phonetics: Anatomy nasal tract (hard) palate velic port oral tract alveolar ridge velum (soft palate) lips tongue teeth pharynx tongue tip glottis(vocal folds and space between vocal cords) vocal folds (larynx) = vocal cords The Speech Production Apparatus(from Olive, p. 23)

  13. Acoustic Phonetics: Anatomy • Breathing and Speech (from Daniloff, chapter 5): • Duration of expiration in soft speech is 2.4 to 3.5 seconds; maximum value (singers, orators) is 15 to 20 seconds without distress. • Louder voice requires inhaling more deeply after expiration; also deeper inhalation if followed by longer speech. • More intense voicing requires greater lung pressure. • Lung pressure relatively constant throughout an utterance. • Emphasis in speech: greater tenseness in vocal folds yielding higher F0; greater lung pressure increases airflow (energy).

  14. Acoustic Phonetics: Anatomy the false vocal folds narrow the glottis during swallowing, preventing pieces of food from getting into the trachea.

  15. Acoustic Phonetics: Anatomy Phonation (from Daniloff, chapter 6): Phonation is “conversion of potential energy of compressed air into kinetic energy of acoustic vibration.” For voiced speech: 1. Buildup of Pressure: air pressure from the lungs pushes against closed vocal folds so that Psubglottal > Poral; buildup continues until until Psubglottal – Poral > elastic recoil force of vocal folds 2. Release: vocal folds forced open by pressure difference; burst of compressed air hits air in vocal tract, causing acoustic shock wave moving along vocal tract

  16. Acoustic Phonetics: Anatomy Phonation 3. Closure of Vocal Folds, two factors: (a) force of elastic recoil in vocal folds Vocal folds have elastic or recoil force proportional to the degree of change from the resting position. (b) Bernoulli Effect (i) energy at location of vocal folds is conserved:E = KE + PE (ii) increase in KE causes decrease in PE (iii) PE corresponds to pressure of air (iv) drop in pressure causes walls of glottis to be drawn closer together Summary: air burst causes high rate of airflow, causes drop in pressure, causes folds to be pulled together

  17. Acoustic Phonetics: Anatomy • Implications: • vocal folds do not open and close because of separate muscle • movements • 2. opening and closing is automatic as long as the resting position • of the vocal folds is (near) closure, and there is sufficient • pressure buildup below vocal folds • 3. Factors governing vocal fold vibration: • (a) position of vocal folds (degree of closeness between folds) • (b) elasticity of vocal folds, depending on position and • degree of tension • (c) degree of pressure drop across vocal folds

  18. Acoustic Phonetics: Anatomy Types of phonation (from Daniloff, p. 194) quiet breathing forced inhalation normal phonation whisper

  19. Acoustic Phonetics: Anatomy The cycle of glottal vibration (from Daniloff, p. 171) 1. folds at rest 2. muscle contraction 5. “explosion” open 6. acoustic shockwave 3. increase in pressure 4. forcing folds apart 7. rebound toward closure 8. folds close, goto step (3)

  20. Acoustic Phonetics: Anatomy The cycle of glottal vibration (from Pickett, p. 50) opening to closure, 2.4 to 4.5 msec closure to opening, 0 to 2.1 msec (F0 = 222 Hz)

  21. Acoustic Phonetics: Anatomy Types of phonation (from Daniloff, p. 174) voiced, creak, glottal stop voiceless, whisper, breathy

  22. Acoustic Phonetics: Anatomy Some cool (gross?) videos: Video of fiberoptic stroboscopy exam: (ignore the background music!) And here’s another video from http://www.voiceinfo.org/ showing the vibration of the vocal folds as a person’s pitch increases: http://www.youtube.com/watch?v=ajbcJiYhFKY

  23. Acoustic Phonetics: Anatomy The effects of nasalization on vowels (from Pickett, p. 71) Figure 4-17. An example of the effects of vowel nasalization on the vowel spectrum. The spectrum envelopes of a normal [a] and a heavily nasalized [a] were plotted… The first three formants are labeled in the normal vowel. In the nasalized vowel, there are three local reductions in spectrum level, indicated by “z’s”; these are the result of the addition of anti-resonant zeros to the vocal tract response, due to a wide-open velar port.

  24. Acoustic Phonetics: Anatomy • The effects of nasalization on vowels (from Pickett, p. 71) • Coupling of the oral and nasal tract introduces pole-zero pairs • (resonances & anti-resonances, occurring in pairs) in the spectrum. • The amount of coupling affects the spacing between each pole • and its corresponding zero, as well as their frequency locations. • The presence of a pole-zero pair increases the apparent bandwidth of the neighboring formants. • The presence of spectral zero below F1 tends to make the location of F1 appear slightly higher (50-100 Hz) than it normally would • If the zero is higher in frequency than its corresponding pole, the net effect is to reduce the amplitude of higher frequencies

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