Mechanism of and threshold biomechanical conditions for falsetto voice onset.

The sound source of a voice is produced by the self-excited oscillation of the vocal folds. In modal voice production, a drastic increase in transglottal pressure after vocal fold closure works as a driving force that develops self-excitation. Another type of vocal fold oscillation with less pronoun...

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Autor principal: Shinji Deguchi
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Publicado: Public Library of Science (PLoS) 2011
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Acceso en línea:https://doaj.org/article/79f0630c8e054204a056791529395351
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spelling oai:doaj.org-article:79f0630c8e054204a0567915293953512021-11-18T06:57:44ZMechanism of and threshold biomechanical conditions for falsetto voice onset.1932-620310.1371/journal.pone.0017503https://doaj.org/article/79f0630c8e054204a0567915293953512011-03-01T00:00:00Zhttps://www.ncbi.nlm.nih.gov/pmc/articles/pmid/21408178/pdf/?tool=EBIhttps://doaj.org/toc/1932-6203The sound source of a voice is produced by the self-excited oscillation of the vocal folds. In modal voice production, a drastic increase in transglottal pressure after vocal fold closure works as a driving force that develops self-excitation. Another type of vocal fold oscillation with less pronounced glottal closure observed in falsetto voice production has been accounted for by the mucosal wave theory. The classical theory assumes a quasi-steady flow, and the expected driving force onto the vocal folds under wavelike motion is derived from the Bernoulli effect. However, wavelike motion is not always observed during falsetto voice production. More importantly, the application of the quasi-steady assumption to a falsetto voice with a fundamental frequency of several hundred hertz is unsupported by experiments. These considerations suggested that the mechanism of falsetto voice onset may be essentially different from that explained by the mucosal wave theory. In this paper, an alternative mechanism is submitted that explains how self-excitation reminiscent of the falsetto voice could be produced independent of the glottal closure and wavelike motion. This new explanation is derived through analytical procedures by employing only general unsteady equations of motion for flow and solids. The analysis demonstrated that a convective acceleration of a flow induced by rapid wall movement functions as a negative damping force, leading to the self-excitation of the vocal folds. The critical subglottal pressure and volume flow are expressed as functions of vocal fold biomechanical properties, geometry, and voice fundamental frequency. The analytically derived conditions are qualitatively and quantitatively reasonable in view of reported measurement data of the thresholds required for falsetto voice onset. Understanding of the voice onset mechanism and the explicit mathematical descriptions of thresholds would be beneficial for the diagnosis and treatment of voice diseases and the development of artificial vocal folds.Shinji DeguchiPublic Library of Science (PLoS)articleMedicineRScienceQENPLoS ONE, Vol 6, Iss 3, p e17503 (2011)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Shinji Deguchi
Mechanism of and threshold biomechanical conditions for falsetto voice onset.
description The sound source of a voice is produced by the self-excited oscillation of the vocal folds. In modal voice production, a drastic increase in transglottal pressure after vocal fold closure works as a driving force that develops self-excitation. Another type of vocal fold oscillation with less pronounced glottal closure observed in falsetto voice production has been accounted for by the mucosal wave theory. The classical theory assumes a quasi-steady flow, and the expected driving force onto the vocal folds under wavelike motion is derived from the Bernoulli effect. However, wavelike motion is not always observed during falsetto voice production. More importantly, the application of the quasi-steady assumption to a falsetto voice with a fundamental frequency of several hundred hertz is unsupported by experiments. These considerations suggested that the mechanism of falsetto voice onset may be essentially different from that explained by the mucosal wave theory. In this paper, an alternative mechanism is submitted that explains how self-excitation reminiscent of the falsetto voice could be produced independent of the glottal closure and wavelike motion. This new explanation is derived through analytical procedures by employing only general unsteady equations of motion for flow and solids. The analysis demonstrated that a convective acceleration of a flow induced by rapid wall movement functions as a negative damping force, leading to the self-excitation of the vocal folds. The critical subglottal pressure and volume flow are expressed as functions of vocal fold biomechanical properties, geometry, and voice fundamental frequency. The analytically derived conditions are qualitatively and quantitatively reasonable in view of reported measurement data of the thresholds required for falsetto voice onset. Understanding of the voice onset mechanism and the explicit mathematical descriptions of thresholds would be beneficial for the diagnosis and treatment of voice diseases and the development of artificial vocal folds.
format article
author Shinji Deguchi
author_facet Shinji Deguchi
author_sort Shinji Deguchi
title Mechanism of and threshold biomechanical conditions for falsetto voice onset.
title_short Mechanism of and threshold biomechanical conditions for falsetto voice onset.
title_full Mechanism of and threshold biomechanical conditions for falsetto voice onset.
title_fullStr Mechanism of and threshold biomechanical conditions for falsetto voice onset.
title_full_unstemmed Mechanism of and threshold biomechanical conditions for falsetto voice onset.
title_sort mechanism of and threshold biomechanical conditions for falsetto voice onset.
publisher Public Library of Science (PLoS)
publishDate 2011
url https://doaj.org/article/79f0630c8e054204a056791529395351
work_keys_str_mv AT shinjideguchi mechanismofandthresholdbiomechanicalconditionsforfalsettovoiceonset
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