2022
DOI: 10.1016/j.chaos.2022.112188
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Controlling chaotic oscillations in a symmetric two-mass model of the vocal folds

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Cited by 7 publications
(3 citation statements)
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“…(1) respectively stand for the identity and zero matrices, while in the first row we get the mass matrix M, the damping matrix C, the stiffness matrix K and the collision matrix Θ. Explicit expressions for them can be found in [4]. The force vector is given by f v = (P 1 Ld 1l , 0) ⊤ , where L is the glottis length, d 1l the thickness of m 1l and P 1 the glottal pressure,…”
Section: Theory 21 Vocal Fold Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…(1) respectively stand for the identity and zero matrices, while in the first row we get the mass matrix M, the damping matrix C, the stiffness matrix K and the collision matrix Θ. Explicit expressions for them can be found in [4]. The force vector is given by f v = (P 1 Ld 1l , 0) ⊤ , where L is the glottis length, d 1l the thickness of m 1l and P 1 the glottal pressure,…”
Section: Theory 21 Vocal Fold Modelmentioning
confidence: 99%
“…It was first proposed in [4], that it might be possible to regulate the chaotic motion of the VFs by means of a theoretical phonation pacemaker attached to one of the model masses and whose parameters could be tuned to alter the energy of the system appropriately [5,6]. In this work we want to explore the effects that the pacemaker might have on the numerical generation of vowel /a/.…”
Section: Introductionmentioning
confidence: 99%
“…Deterministic chaos makes the spectrum noisy, and the distorted harmonics in high-pitched vocalizations are easily mistaken for formants on spectrograms [21]. As a result, it is often assumed that chaos would make vowels difficult to recognize [58], but again we are not aware of any perceptual data to confirm this.…”
Section: Introductionmentioning
confidence: 99%