Number of the records: 1  

Acoustic perturbation equations and Lighthill's acoustic analogy for the human phonation

  1. 1.
    SYSNO ASEP0394350
    Document TypeJ - Journal Article
    R&D Document TypeJournal Article
    Subsidiary JOstatní články
    TitleAcoustic perturbation equations and Lighthill's acoustic analogy for the human phonation
    Author(s) Zoerner, S. (AT)
    Šidlof, Petr (UT-L) RID
    Huppe, A. (AT)
    Kaltenbacher, M. (AT)
    Source TitleProceedings of Meetings on Acoustics -ICA 2013, 19. - Montreal : Acoustical Society of America, 2013 - ISSN 1939-800X
    Roč. 19, 060309 (2013), s. 1-8
    Number of pages8 s.
    Publication formOnline - E
    ActionICA 2013 - Meetings on Acoustics
    Event date02.06.2013-07.06.2013
    VEvent locationMontreal
    CountryCA - Canada
    Event typeWRD
    Languageeng - English
    CountryCA - Canada
    Keywordsvocal folds ; CFD ; computational aeroacoustics
    Subject RIVBI - Acoustics
    R&D ProjectsGAP101/11/0207 GA ČR - Czech Science Foundation (CSF)
    Institutional supportUT-L - RVO:61388998
    DOI10.1121/1.4799392
    AnnotationIn speech, air is driven through the larynx by compression of the lungs. Thereby, air flows through the glottis which forces the vocal folds to oscillate which in turn results in a pulsating air flow. This air flow is the main source of the generated sound-the phonation. The acoustic wave then passes through the vocal tract, which acts as a filter modulating the propagated sound leaving the mouth. We model the fluid-structureacoustic interaction with a so called hybrid approach. The air flow in the larynx, together with a prescribed vocal fold motion, is simulated with help of the open source solver OpenFOAM. Based on the resulting fluid field, acoustic source terms and the wave propagation is calculated within the finite element solver CFS++. Two methods are available to choose from, Lighthill's acoustic analogy and an aeroacoustic analogy based on a perturbation ansatz. Additionally, the simulation domain is extended by a realistic but geometrical fixed vocal tract and connected to a propagation region. The different acoustic approaches are compared, by analysing the acoustic pressure in the glottis (source region) and outside the vocal tract. Moreover, to illustrate the effects of the vocal tract an alternative geometry is used for comparison.
    WorkplaceInstitute of Thermomechanics
    ContactMarie Kajprová, kajprova@it.cas.cz, Tel.: 266 053 154 ; Jana Lahovská, jaja@it.cas.cz, Tel.: 266 053 823
    Year of Publishing2014
Number of the records: 1  

  This site uses cookies to make them easier to browse. Learn more about how we use cookies.