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               <dc:title>Influence of vocal tract geometry simplifications on the numerical simulation of vowel sounds</dc:title>
               <dc:creator>Arnela, Marc</dc:creator>
               <dc:creator>Dabbaghchian, Saeed</dc:creator>
               <dc:creator>Bladin, Rémi</dc:creator>
               <dc:creator>Guasch, Oriol</dc:creator>
               <dc:creator>Engwall, Olov</dc:creator>
               <dc:creator>Van Hirtum, Annemie</dc:creator>
               <dc:creator>Pelorson, Xavier</dc:creator>
               <dc:subject>Vocal tract acoustics</dc:subject>
               <dc:subject>Human voice</dc:subject>
               <dc:subject>Acoustical properties</dc:subject>
               <dc:subject>Acoustic field</dc:subject>
               <dc:subject>Vowel systems</dc:subject>
               <dc:subject>Wave propagation</dc:subject>
               <dc:subject>Computer simulation</dc:subject>
               <dc:subject>Finite-element analysis</dc:subject>
               <dc:subject>Partial differential equations</dc:subject>
               <dc:subject>Organs</dc:subject>
               <dc:description>For many years, the vocal tract shape has been approximated by one-dimensional (1D) area functions to study the production of voice. More recently, 3D approaches allow one to deal with the complex 3D vocal tract, although area-based 3D geometries of circular cross-section are still in use. However, little is known about the influence of performing such a simplification, and some alternatives may exist between these two extreme options. To this aim, several vocal tract geometry simplifications for vowels [ɑ], [i], and [u] are investigated in this work. Six cases are considered, consisting of realistic, elliptical, and circular cross-sections interpolated through a bent or straight midline. For frequencies below 4–5 kHz, the influence of bending and cross-sectional shape has been found weak, while above these values simplified bent vocal tracts with realistic cross-sections are necessary to correctly emulate higher-order mode propagation. To perform this study, the finite element method (FEM) has been used. FEM results have also been compared to a 3D multimodal method and to a classical 1D frequency domain model.</dc:description>
               <dc:date>2015-12-17</dc:date>
               <dc:date>2016-09-15</dc:date>
               <dc:type>info:eu-repo/semantics/article</dc:type>
               <dc:identifier>0001-4966</dc:identifier>
               <dc:identifier>http://hdl.handle.net/20.500.14342/5729</dc:identifier>
               <dc:identifier>https://doi.org/10.1121/1.4962488</dc:identifier>
               <dc:language>eng</dc:language>
               <dc:relation>Journal of the Acoustical Society of America (2016), Vol. 140, Nº3, pp 1707-1718</dc:relation>
               <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
               <dc:rights>© Acoustical Society of America. Tots els drets reservats</dc:rights>
               <dc:publisher>Acoustical Society of America</dc:publisher>
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