Physical Medicine and Rehabilitation, Johns Hopkins University , Baltimore, Maryland.
Department of Cognitive Biology, University of Vienna , Vienna , Austria.
J Appl Physiol (1985). 2018 Jan 1;124(1):34-39. doi: 10.1152/japplphysiol.00902.2016. Epub 2017 Aug 24.
The fluid mechanics of whistling involve the instability of an air jet, resultant vortex rings, and the interaction of these rings with rigid boundaries (see http://www.canal-u.tv/video/cerimes/etude_radiocinematographique_d_un_siffleur_turc_de_kuskoy.13056 and Meyer J. Whistled Languages. Berlin, Germany: Springer, 2015, p. 74-774). Experimental models support the hypothesis that the sound in human whistling is generated by a Helmholtz resonator, suggesting that the oral cavity acts as a resonant chamber bounded by two orifices, posteriorly by raising the tongue to the hard palate, and anteriorly by pursed lips (Henrywood RH, Agarwal A. Phys Fluids 25: 107101, 2013). However, the detailed anatomical changes in the vocal tract and their relation to the frequencies generated have not been described in the literature. In this study, videofluoroscopic and simultaneous audio recordings were made of subjects whistling with the bilabial (i.e., "puckered lip") technique. One whistling subject was also recorded, using magnetic resonance imaging. As predicted by theory, the frequency of sound generated decreased as the size of the resonant cavity increased; this relationship was preserved throughout various whistling tasks and was consistent across subjects. Changes in the size of the resonant cavity were primarily modulated by tongue position rather than jaw opening and closing. Additionally, when high-frequency notes were produced, lateral chambers formed in the buccal space. These results provide the first dynamic anatomical evidence concerning the acoustic production of human whistling. NEW & NOTEWORTHY We establish a new and much firmer quantitative and physiological footing to current theoretical models on human whistling. We also document a novel lateral airflow mechanism used by both of our participants to produce high-frequency notes.
吹气口哨的流体力学涉及不稳定的射流、产生的涡环以及这些环与刚性边界的相互作用(请参见 http://www.canal-u.tv/video/cerimes/etude_radiocinematographique_d_un_siffleur_turc_de_kuskoy.13056 和 Meyer J. Whistled Languages. Berlin, Germany: Springer, 2015, p. 74-774)。实验模型支持了这样一种假设,即人类口哨声是由亥姆霍兹共鸣器产生的,这表明口腔充当了一个共鸣腔,由两个孔口限定,后面由舌头抬高到硬腭,前面由嘴唇紧闭形成(Henrywood RH, Agarwal A. Phys Fluids 25: 107101, 2013)。然而,有关声道的详细解剖变化及其与产生的频率之间的关系尚未在文献中描述。在这项研究中,对使用双唇(即“噘嘴”)技术吹口哨的受试者进行了视频荧光透视和同时音频记录。还对一位口哨受试者进行了磁共振成像记录。正如理论预测的那样,随着共鸣腔尺寸的增加,产生的声音频率降低;这种关系在各种口哨任务中都保持不变,并且在受试者之间也一致。共鸣腔的大小变化主要由舌头位置调节,而不是由颌部的张开和闭合调节。此外,当产生高频音符时,颊腔会形成侧向腔室。这些结果为人类口哨声的声学产生提供了第一个动态解剖学证据。新的和值得注意的是,我们为当前关于人类口哨的理论模型建立了一个新的、更坚实的定量和生理学基础。我们还记录了我们的两位参与者用来产生高频音符的一种新颖的侧向气流机制。