ArticleThe Journal of the Acoustical Society of America2017
Comparison of a fiber-gel finite element model of vocal fold vibration to a transversely isotropic stiffness model.
Article in The Journal of the Acoustical Society of America, 2017. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 7 papers.
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Who cites it
7 citing papers in PubMed.
- Vocal Tradeoffs in Anterior Glottoplasty for Voice Feminization.The Laryngoscope · 2021Article
- Effect of Vocal Fold Implant Placement on Depth of Vibration and Vocal Output.The Laryngoscope · 2020Article
- Mapping Thyroarytenoid and Cricothyroid Activations to Postural and Acoustic Features in a Fiber-Gel Model of the Vocal Folds.Applied sciences (Basel, Switzerland) · 2019Article
- Sensitivity analysis of muscle mechanics-based voice simulator to determine gender-specific speech characteristics.Biomechanics and modeling in mechanobiology · 2019Article
- A computational study of depth of vibration into vocal fold tissues.The Journal of the Acoustical Society of America · 2019Article
- WHERE HAS ALL THE POWER GONE? ENERGY PRODUCTION AND LOSS IN VOCALIZATION.Speech communication · 2018Article
- Vocal fold contact patterns based on normal modes of vibration.Journal of biomechanics · 2018Article
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Authors and funding
4 authors.
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Abstract
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.
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