Ja n 20 02 Modeling Vocal Fold Motion with a New Hydrodynamic Semi-Continuum Model

Vocal fold (VF) motion is a fundamental process in voice production, and is also a challenging problem for direct numerical computation because the VF dynamics depend on nonlinear coupling of air flow with the response of elastic channels (VF), which undergo opening and closing, and induce internal flow separation. A traditional modeling approach makes use of steady flow approximation or Bernoulli’s law which is known to be invalid during VF opening. We present a new hydrodynamic semi-continuum system for VF motion. The airflow is modeled by a quasi-one dimensional continuum aerodynamic system, and the VF by a classical lumped two mass system. The reduced flow system contains the Bernoulli’s law as a special case, and is derivable from the two dimensional compressible Navier-Stokes equations. Since we do not make steady flow approximation, we are able to capture transients and rapid changes of solutions, e.g. the double pressure peaks at opening and closing stages of VF motion consistent with experimental data. We demonstrate numerically that our system is robust, and models in-vivo VF oscillation more physically. It is also much simpler than a full two-dimensional Navier-Stokes system. PACS numbers: 43.70Bk, 43.28Ra, 43.28Py, 43.40Ga.

[1]  I R Titze,et al.  Observation of perturbations in a lumped-element model of the vocal folds with application to some pathological cases. , 1991, The Journal of the Acoustical Society of America.

[2]  J. Flanagan Speech Analysis, Synthesis and Perception , 1971 .

[3]  J. Flanagan,et al.  Synthesis of voiced sounds from a two-mass model of the vocal cords , 1972 .

[4]  M. Mcpherson,et al.  Introduction to fluid mechanics , 1997 .

[5]  Coarticulation • Suprasegmentals,et al.  Acoustic Phonetics , 2019, The SAGE Encyclopedia of Human Communication Sciences and Disorders.

[6]  R. LeVeque Numerical methods for conservation laws , 1990 .

[7]  I. Titze,et al.  Measurement of vocal fold intraglottal pressure and impact stress. , 1994, Journal of voice : official journal of the Voice Foundation.

[8]  I R Titze,et al.  The effect of subglottal resonance upon vocal fold vibration. , 1997, Journal of voice : official journal of the Voice Foundation.

[9]  I. Titze Current topics in voice production mechanisms. , 1993, Acta oto-laryngologica.

[10]  A.P. Benguerel,et al.  Speech analysis , 1981, Proceedings of the IEEE.

[11]  Tai-Ping Liu Nonlinear stability and instability of transonic flows through a nozzle , 1982 .

[12]  Shock wave driven by a phased implosion , 1991 .

[13]  G. Berke,et al.  The effect of laryngeal nerve stimulation on phonation: a glottographic study using an in vivo canine model. , 1988, The Journal of the Acoustical Society of America.

[14]  Tai-Ping Liu Transonic gas flow in a duct of varying area , 1982 .

[15]  I. Titze,et al.  Voice simulation with a body-cover model of the vocal folds. , 1995, The Journal of the Acoustical Society of America.

[16]  I. Titze The physics of small-amplitude oscillation of the vocal folds. , 1988, The Journal of the Acoustical Society of America.

[17]  D. Berry,et al.  A finite-element model of vocal-fold vibration. , 2000, The Journal of the Acoustical Society of America.

[18]  C. R. Illingworth,et al.  On the Human Voice , 1876, Edinburgh medical journal.

[19]  E. Luschei,et al.  Effect of Subglottic Pressure on Fundamental Frequency of the Canine Larynx with Active Muscle Tensions , 1994, The Annals of otology, rhinology, and laryngology.

[20]  C H Coker,et al.  Characteristics of a pulsating jet through a small modulated orifice, with application to voice production. , 1997, The Journal of the Acoustical Society of America.

[21]  I R Titze,et al.  The Human Vocal Cords: A Mathematical Model , 1974, Phonetica.