Part 2 Acoustics of Consonants Flashcards
Theory of Fricative Acoustics
Obstruents are produced with a noise source, usually located in the vicinity of the major constriction or at the point where an obstacle (e.g., the teeth) interrupts airflow within the vocal tract
⦁ Noise sources are aperiodic
⦁ In cases where the obstruent is voiced,
the voicing source occurs simultaneously with the vocal tract noise source
⦁ Mixed sources
Laminar airflow
Laminar airflow within a tube. Laminar airflow is indicated by the parallel lines ending in arrowheads. Because pressure at the left of the tube (P1) is greater than pressure at the right of the tube (Pr), air flows from left to right, toward the lower pressure.
Fluid Flow
As the air molecules enter the constriction they undergo an increase in speed.
⦁ They “shoot out” of the constriction exit in the form of a narrow stream or jet which expands as it moves downstream, toward the end of the tube.
⦁ The jet of air emerges from the constriction as a group of narrowly focused parallel lines.
⦁ There are also circular motions of air molecules along the edges of the jet.
⦁ turbulent flow, or turbulence.
Fricative Production
Turbulence generated at the exit
Turbulence generated at the exit of the supralaryngeal (above the larynx and within the vocal tract) constrictions results in a frication source
Source of sound in fricatives represents
Source of sound in fricatives represents a transformation of aeromechanical energy (in the form of turbulent flows) to acoustic energy (in the form of aperiodic waveforms and their spectra).
⦁ The tube model shows how air flowing through a constriction leads to the formation of a jet, around which turbulent flow is generated.
⦁ Air flows through a constriction because there
is a pressure differential across it. In fricative
production, pressure is higher in back of the
constriction than in front of it.
Mixed Sources in Fricative Production
⦁ Production of the English fricatives /v/, /ð/, /z/, and /ʒ/ involves
Production of the English fricatives /v/, /ð/, /z/, and /ʒ/ involves turbulence, but may also be accompanied by vibration of the vocal folds
⦁ These voiced fricatives are produced with two types of sources
⦁ the aperiodic, turbulent flow generated in the vocal tract
⦁ The periodic vibration of the vocal folds
⦁ When there is a mixed source, both source spectra
are shaped by the resonant characteristics of the vocal tract
Shaping of Fricative Sources by Vocal Tract Resonators
The narrow vocal tract constriction require
The narrow vocal tract constriction required for fricatives divides the vocal tract into a front and back cavity.
The source energy, located close to the constriction or in front of the constriction (e.g., at the teeth), is propagated in both directions along the long axis of the vocal tract
⦁ . Both the front and back cavities shape the source spectrum.
Shaping of Fricative Sources by Vocal Tract Resonators cont.
The back cavity shapes
⦁ The front cavity, being open to the atmosphere, shapes the source spectrum by emphasizing a frequency region of the spectrum.
⦁ The emphasized frequencies appear in the output spectrum as high-amplitude regions, or broad peaks across a range of frequencies
The back cavity shapes the source spectrum by introducing antiresonances into the fricative output spectrum.
Rule for Fricative Spectra
As the cavity in front of the constriction gets smaller, the resonances of the frication spectra move to higher frequencies.
⦁ This is consistent with the idea that air volumes in smaller resonating cavities are stiffer than air volumes in larger cavities.
⦁ As the cavity behind the constriction gets smaller, the resonant frequency of the antiresonances increases for the same reason.
Measurement of Fricative Acoustics
⦁
The goal of a measurement strategy for fricative spectra is to obtain a set of numbers, that reliably distinguishes between fricatives having different places of articulation, and possibly even between fricatives having the same place of articulation but different voicing characteristics.
⦁
(no standard method, like F-patterns for vowels)
Theory of Stop Acoustics
Airflow in a tube with a complete constriction in the tube (arrow) that prevents air from passing through to the right side.
⦁ Pressure builds up behind the constriction, as is the case for stop consonants. P1 is the pressure behind the constriction and Pr is the reference pressure (atmospheric pressure).
Articulation of Stop Consonants
During speech production, completely closed tubes occur for the articulation of stop consonants.
The complete blockage of airflow for stops may be formed at several places throughout the vocal tract
⦁ In connected speech these complete blockages last no longer than about 100 ms (1/10 of a second)
Articulation of Stop Consonants
Air molecules behind the stop construction
Air molecules behind the stop constriction are compressed simultaneously and uniformly
Nasal cavities are excluded from this volume because the velopharyngeal port is closed for production of stops (and all English obstruents)
Air Compression for Voiced & Voiceless Stops
⦁
Air compression during voiceless stop ⦁ The peak (highest) value of Po is
equivalent to the peak values of Pt and Palv because the vocal folds are abducted
⦁ Air compression during voiced stop
⦁ Peak value of Po does not equal Pt and
Palv because as air flows through the
vibrating vocal folds there is some loss
of pressure.
⦁ Resulting in Po values that are generally
Voiceless & Voiced Stops
A. (/t/) Oral, tracheal, and alveolar air pressures are equal during the stop closure interval.
⦁ B. (/d/) Air is compressed only in the spaces between the stop constriction and the larynx. Tracheal air pressure is greater than oral air pressure and both are greater than atmospheric air pressure