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Comparison of a fiber-gel finite element model of vocal fold vibration to a transversely isotropic stiffness model

机译:声带振动的纤维-凝胶有限元模型与横观各向同性刚度模型的比较

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摘要

A fiber-gel vocal fold model is compared to a transversely isotropic stiffness model in terms of normal mode vibration. The fiber-gel finite element model (FG-FEM) consists of a series of gel slices, each with a two-dimensional finite element mesh, in a plane transverse to the tissue fibers. The gel slices are coupled with fibers under tension in the anterior-posterior dimension. No vibrational displacement in the fiber-length direction is allowed, resulting in a plane strain state. This is consistent with the assumption of transverse displacement of a simple string, offering a wide range of natural frequencies (well into the kHz region) with variable tension. For low frequencies, the results compare favorably with the natural frequencies of a transversely isotropic elastic stiffness model (TISM) in which the shear modulus in the longitudinal plane is used to approximate the effect of fiber tension. For high frequencies, however, the natural frequencies do not approach the string mode frequencies unless plane strain is imposed on the TISM model. The simplifying assumption of plane strain, as well as the use of analytical closed-form shape functions, allow for substantial savings in computational time, which is important in clinical and exploratory applications of the FG-FEM model.
机译:就正常模式振动而言,将纤维凝胶声带折模型与横向各向同性刚度模型进行了比较。纤维-凝胶有限元模型(FG-FEM)由一系列凝胶切片组成,每个凝胶切片均在与组织纤维垂直的平面中具有二维有限元网格。凝胶片在前后尺寸的张力下与纤维耦合。不允许沿纤维长度方向的振动位移,从而导致平面应变状态。这与简单弦的横向位移的假设是一致的,它提供了可变张力的宽范围的固有频率(进入kHz区域)。对于低频,结果与横向各向同性的弹性刚度模型(TISM)的固有频率相比非常好,在横向模型中,纵向方向的剪切模量用于近似纤维张力的影响。但是,对于高频,除非在TISM模型上施加平面应变,否则固有频率不会接近弦模式频率。平面应变的简化假设以及分析性封闭形式的形状函数的使用,可以节省大量的计算时间,这在FG-FEM模型的临床和探索性应用中很重要。

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