{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,2,28]],"date-time":"2026-02-28T18:46:31Z","timestamp":1772304391498,"version":"3.50.1"},"reference-count":74,"publisher":"Acoustical Society of America (ASA)","issue":"5","content-domain":{"domain":["pubs.aip.org"],"crossmark-restriction":true},"short-container-title":[],"published-print":{"date-parts":[[2023,11,1]]},"abstract":"<jats:p>According to nonlinear source-filter theory, as the strength of the coupling between the source and filter increases, typically by a decrease in the vocal tract cross-sectional area, the resultant increase in the inertance of the vocal tract yields an increase in the interactions between acoustic pressures within the vocal tract and the changing glottal airflow and\/or the vibratory pattern of the vocal folds as noted in Titze [(2008). J. Acoust. Soc. Am. 123(4), 1902\u20131915]. The purpose of the current research was to examine the effects of parametric vocal tract constrictions mimicking epilaryngeal tube and lip narrowing on aerodynamic measures in a dynamic self-oscillating physical model of the vocal folds and vocal tract. Multilayered silicone vocal fold models were created based on Murray and Thomson [(2011). J. Visualized Exp. 58, e3498] and Murray and Thomson [(2012). J. Acoust. Soc. Am. 132(5), 3428\u20133438] and mounted to a simple synthetic trachea and supraglottal vocal tract model. Four constriction cross-sectional areas were examined at two locations (i.e., at the epilarynx and lip regions). Phonation threshold pressure and flow were measured at phonation onset and offset using four M5-CONV vocal fold models. Results indicated that both constriction magnitude and location are relevant factors in determining glottal aerodynamics. In general, a narrow epilarynx tube or lip constriction resulted in the lowest onset pressures and airflows while the no vocal tract condition resulted in the highest onset pressures and airflows.<\/jats:p>","DOI":"10.1121\/10.0022383","type":"journal-article","created":{"date-parts":[[2023,11,20]],"date-time":"2023-11-20T19:27:32Z","timestamp":1700508452000},"page":"3310-3320","update-policy":"https:\/\/doi.org\/10.1063\/aip-crossmark-policy-page","source":"Crossref","is-referenced-by-count":2,"title":["The effects of vocal tract constrictions on aerodynamic measures in a synthetic vocal fold model"],"prefix":"10.1121","volume":"154","author":[{"given":"Nicholas A.","family":"May","sequence":"first","affiliation":[{"name":"The University of Maine 1 , Orono, Maine 04469, USA"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-4520-925X","authenticated-orcid":false,"given":"Ronald C.","family":"Scherer","sequence":"additional","affiliation":[{"name":"Bowling Green State University 2 , Bowling Green, Ohio 43404, USA"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"231","published-online":{"date-parts":[[2023,11,20]]},"reference":[{"key":"2023112019271334200_c1","article-title":"Effects of false vocal fold width on translaryngeal flow resistance","year":"2004"},{"key":"2023112019271334200_c2","doi-asserted-by":"publisher","first-page":"36","DOI":"10.1016\/j.jvoice.2015.02.004","article-title":"The flow and pressure relationships in different tubes commonly used for semi-occluded vocal tract exercises","volume":"30","year":"2016","journal-title":"J. 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