UCLA School of Medicine, 31-24 Rehabilitation Center, 1000 Veteran Avenue, Los Angeles, CA 90095-1794, USA.
J Acoust Soc Am. 2010 Apr;127(4):2554-62. doi: 10.1121/1.3308410.
Previous studies show that phonation onset occurs as two eigenmodes of the vocal folds are synchronized by the interaction between the vocal folds and the glottal flow. This study examines the influence of the geometrical and biomechanical properties of the vocal folds on this eigenmode-synchronization process, with a focus on phonation threshold pressure and frequency. The analysis showed that phonation threshold pressure was determined by the frequency spacing and coupling strength between the two natural modes that were synchronized by the fluid-structure interaction. The phonation frequency at onset was the root mean square value of the two natural frequencies plus a correction due to the added stiffness of the glottal flow. When higher-order modes of the vocal fold structure were included, more than one group of eigenmodes was synchronized as the system moved toward phonation onset. Changes in vocal fold biomechanics may change the relative dominance between different groups and cause phonation onset to occur at a different eigenmode, which was often accompanied by an abrupt change in onset frequency. Due to the synchronization of multiple pairs of eigenmodes and the mode-switching possibility, a complete and accurate description of vocal fold biomechanical properties is needed to determine the final synchronization pattern and obtain a reliable calculation of the dependence of phonation threshold pressure and frequency on vocal fold geometry and other biomechanical properties.
先前的研究表明,声带的两个本征模态通过声带和气流之间的相互作用同步,发声起始发生于此。本研究考察了声带的几何和生物力学特性对这一本征模态同步过程的影响,重点关注发声起始压和频率。分析表明,发声起始压由通过流固耦合同步的两个自然模态的频率间隔和耦合强度决定。起始发声频率是两个自然频率的均方根值加上由于声门流附加刚度引起的校正值。当包括声带结构的高阶模态时,随着系统向发声起始移动,会有超过一组本征模态被同步。声带生物力学的变化可能会改变不同组之间的相对优势,并导致发声起始发生在不同的本征模态,这通常伴随着起始频率的突然变化。由于多对本征模态的同步和模式切换的可能性,需要对声带生物力学特性进行完整和准确的描述,以确定最终的同步模式,并获得发声起始压和频率对声带几何形状和其他生物力学特性的可靠计算。