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The Effects of the False Vocal Fold Gaps in a Model of the Larynx on Pressures Distributions and Flows

机译:虚假声折叠间隙在压力分布和流量的喉部模型中的影响

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Human phonation does not merely depend upon the vibration of the vocal folds. The false vocal fold (FVF), as an important laryngeal constriction, has also been found by more and more research both in clinically and computer simulations that it plays an important role during phonation and contributes significantly to the aerodynamics and sound generation processes of human voice production. Among many parameters which are used to determine and describe the geometry of the false vocal folds, the false vocal fold gap (GFVF), which means the minimal distance between the two false vocal folds, is regarded as an important and dominant parameter. Therefore, this study explores the effects of the FVF gaps on the intralaryngeal pressure distributions, laryngeal resistance and flows using both three-dimensional Plexiglas model and commercially available computational fluid dynamics code. Three glottal angles, divergent 40°, uniform 0°, and convergent -40°were used for this study to explore the effects of FVF gaps, as they represent the basic glottal shapes typically expected in phonation, the angle values also were typically expected for most phonation in modal Register. A wide variety of FVF gaps (GFVF) were parameterized with 12 different values: 0.02, 0.04, 0.06, 0.08, 0.09, 0.1, 0.11, 0.12, 0.16, 0.2, 0.4, 0.6 cm to represent important geometries often appearing within phonatory vibratory cycles. These gaps were used for each glottal angle. The specific design of the FVFs followed prior literature. The minimal glottal diameter (Dg) was constantly at 0.06 cm in this study for each FVF gaps, and the translaryngeal pressure were held constant at 8 cm H2O. A nonvibrating laryngeal airway Plexiglas model, which had linear dimensions 1.732 times of a normal male larynx, was used in this study. In order to measure pressures inside the Plexiglas model, twelve cylindrical ducts were made on the midline of the laryngeal wall of the model. The diameter of each duct was 0.07 cm human size (0.12 cm in the model), so that the connector of an Entran EPE-551 pressure transducer could fit snugly into the holes. The distance between the centers of each hole was 0.14 cm human size. FLUENT (Fluent, Inc., Lebanon, NH), a commercially available computational fluid dynamics code was also used to obtain estimates of the normal wall pressures along the laryngeal surfaces (including the surfaces of vocal folds, ventricles, and false vocal folds) as a function of the FVF gaps and the glottal angles.
机译:人类发声并不仅仅取决于声带的振动。假声带(FVF),作为一种重要的喉部收缩,还发现通过以上的水平,临床和计算机模拟更多的研究都认为它发声,并有助于显著的空气动力学和人声的声音产生过程中起着重要的作用生产。其中用于确定和描述了假声带的几何形状的许多参数,假声带间隙(GFVF),这意味着在两个假声襞之间的最小距离,被认为是一个重要的和主导参数。因此,本研究探讨了在喉内压力分布,喉癌电阻FVF间隙的影响,并同时使用三维模型有机玻璃和市售计算流体动力学代码流动。三个声门角度,发散40°,均匀的0°,并会聚-40°用于该研究,探索FVF间隙的影响,因为它们代表了基本声门形状通常预期在发声,角度值也被典型地用于预期最发声模态注册。各种各样FVF间隙(GFVF)与12个不同的值被参数化:0.02,0.04,0.06,0.08,0.09,0.1,0.11,0.12,0.16,0.2,0.4,0.6厘米到表示经常出现发声振动周期内重要的几何形状。这些间隙用于每个声门角。所述FVFs的具体设计遵循现有文献。最小直径声门(DG)是恒定在0.06厘米在该研究中对于每个FVF间隙,并且所述translaryngeal压力物在8厘米H2O保持恒定。甲nonvibrating喉部气道有机玻璃模型,其具有线性的尺寸的正常男性喉的1.732倍,在该研究中使用。为了测量树脂玻璃模型内的压力,12个圆筒状管道中对模型的喉部壁的中线制成。每个导管的直径为0.07厘米人类尺寸(0.12厘米的模型),使得ENTRAN EPE-551压力换能器的连接器可紧贴地配合到孔中。每个孔的中心之间的距离为0.14厘米人类大小。 FLUENT(流利公司,黎巴嫩,NH),可商购的计算流体动力学代码也被用于获得沿着喉表面(包括声带,脑室,假声带的表面)的正常壁压力作为估计的FVF差距和声门角度的函数。

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