Abstract

Recently, 3D printing has been increasingly used to create physical models of the vocal tract with geometries obtained from magnetic resonance imaging. These printed models allow measuring the vocal tract transfer function, which is not reliably possible in vivo for the vocal tract of living humans. The transfer functions enable the detailed examination of the acoustic effects of specific articulatory strategies in speaking and singing, and the validation of acoustic plane-wave models for realistic vocal tract geometries in articulatory speech synthesis. To measure the acoustic transfer function of 3D-printed models, two techniques have been described: (1) excitation of the models with a broadband sound source at the glottis and measurement of the sound pressure radiated from the lips, and (2) excitation of the models with an external source in front of the lips and measurement of the sound pressure inside the models at the glottal end. The former method is more frequently used and more intuitive due to its similarity to speech production. However, the latter method avoids the intricate problem of constructing a suitable broadband glottal source and is therefore more effective. It has been shown to yield a transfer function similar, but not exactly equal to the volume velocity transfer function between the glottis and the lips, which is usually used to characterize vocal tract acoustics. Here, we revisit this method and show both, theoretically and experimentally, how it can be extended to yield the precise volume velocity transfer function of the vocal tract.

Highlights

  • The vocal tract transfer function, i.e., the complex frequency-dependent ratio of the volume velocity at the lips to the volume velocity through the glottis, is widely used to characterize the acoustics of the vocal tract

  • In this paper we presented a precise method for the measurement of the volume velocity transfer function of 3D-printed models of the vocal tract based on acoustic excitation with an external sound source, which avoids the obstacles and limitations involved in transfer function measurements with a glottal source, requires little special equipment, and is simple to conduct

  • This method is an extension of the approach presented by Kitamura et al [10] and has the advantage that the relative levels of the measured resonance peaks correspond to those of the true volume velocity transfer function, and that the overall level of the transfer function corresponds to the true level

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Summary

Introduction

The vocal tract transfer function, i.e., the complex frequency-dependent ratio of the volume velocity (or alternatively sound pressure) at the lips to the volume velocity through the glottis, is widely used to characterize the acoustics of the vocal tract. It contains the information about the frequencies and bandwidths of the formants (resonances), which are of primary importance in many studies. Besides the formants, most transfer functions contain additional. Measurement of vocal tract transfer function and analysis, decision to publish, or preparation of the manuscript

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