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声门启闭压和弹性剪切模量:两质量模型计算与实验的比较。

Phonation threshold pressure and the elastic shear modulus: comparison of two-mass model calculations with experiments.

机构信息

Department of Physics and Astronomy, Bowling Green State University, Bowling Green, Ohio 43403, USA.

出版信息

J Acoust Soc Am. 2012 Oct;132(4):2582-91. doi: 10.1121/1.4747618.

DOI:10.1121/1.4747618
PMID:23039451
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3477191/
Abstract

Ishizaka and Flanagan's classic two-mass model of vocal fold motion is applied to small oscillations where the equations become linear and the aerodynamic driving force is described by an effective stiffness. The solution of these equations includes an analytic formula for the two eigenfrequencies; this shows that conjugate imaginary parts of the frequencies emerge beyond eigenvalue synchronization and that one of the imaginary parts becomes zero at a pressure signaling the instability associated with the onset of threshold. Using recent measurements by Fulcher et al. of intraglottal pressure distributions [J. Acoust. Soc. Am. 129, 1548-1553 (2011).] to inform the behavior of the entrance loss coefficients, an analytic formula for threshold pressure is derived. It fits most of the measurements Chan and Titze reported for their 2006 physical model of the vocal fold mucosa. Two sectors of the mass-stiffness parameter space are used to produce these fits. One is based on a rescaling of the typical glottal parameters of the original Ishizaka and Flanagan work. The second requires setting two of the spring constants equal and should be closer to the experimental conditions. In both cases, values of the elastic shear modulus are calculated from the spring constants.

摘要

伊势崎和弗拉纳根的经典声带运动两质量模型应用于小振动,此时方程变为线性,气动驱动力由有效刚度描述。这些方程的解包括两个特征频率的解析公式;这表明,在特征值同步之外会出现共轭虚部,并且在压力达到标志与阈相关的不稳定性开始的信号时,其中一个虚部变为零。利用富勒等人最近对声门内压力分布的测量[J.声学学会杂志,129,1548-1553(2011)。]来告知入口损耗系数的行为,推导出了阈压的解析公式。它适用于陈和泰兹为他们 2006 年的声带黏膜物理模型报告的大部分测量值。使用两个质量-刚度参数空间的部分来生成这些拟合。一个基于原始伊势崎和弗拉纳根工作中典型声门参数的比例缩放。第二个需要将两个弹簧常数设置为相等,并且应该更接近实验条件。在这两种情况下,从弹簧常数计算弹性剪切模量的值。

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本文引用的文献

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J Acoust Soc Am. 2011 Sep;130(3):1597-605. doi: 10.1121/1.3605672.
2
On the difference between negative damping and eigenmode synchronization as two phonation onset mechanisms.论负阻尼与本征模同步作为两种起始发声机制的区别。
J Acoust Soc Am. 2011 Apr;129(4):2163-7. doi: 10.1121/1.3543989.
3
Pressure distributions in a static physical model of the uniform glottis: entrance and exit coefficients.声门均匀静态物理模型中的压力分布:入口和出口系数。
J Acoust Soc Am. 2011 Mar;129(3):1548-53. doi: 10.1121/1.3514424.
4
Phonation threshold pressure predictions using viscoelastic properties up to 1,400 Hz of injectables intended for Reinke's space.用于 Reinke 空间的注射剂在 1400Hz 以下的粘弹性预测发音阈值压力。
Laryngoscope. 2010 May;120(5):995-1001. doi: 10.1002/lary.20877.
5
Characteristics of phonation onset in a two-layer vocal fold model.双层声带模型中发声起始的特征
J Acoust Soc Am. 2009 Feb;125(2):1091-102. doi: 10.1121/1.3050285.
6
A simple-shear rheometer for linear viscoelastic characterization of vocal fold tissues at phonatory frequencies.一种用于在发声频率下对声带组织进行线性粘弹性表征的简单剪切流变仪。
J Acoust Soc Am. 2008 Aug;124(2):1207-19. doi: 10.1121/1.2946715.
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Physical mechanisms of phonation onset: a linear stability analysis of an aeroelastic continuum model of phonation.发声起始的物理机制:发声气动弹性连续体模型的线性稳定性分析
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