Sound fields in generally shaped curved ear canals.

The sound field in the external ear can be subdivided into a distinctly three-dimensional part in front of pinna and concha, a fairly regular part in the core region of ear canals, and a less regular part in the drum coupling region near the tympanic membrane. The different parts of the sound field and their interaction have been studied using finite elements. A "pinna box" enclosing the pinna provides both a realistic coupling of the external space to the ear canal and the generation of sound. The sound field in the core region turns out to be not that regular as mostly assumed: near pressure minima and maxima "one-sided" isosurfaces (surfaces of equal pressure magnitude) occur, which are inconsistent with the notion of a middle axis, in principle. Nevertheless such isosurfaces can be seen as part of a "fundamental sound field," which is governed by the principle of minimum energy. Actually, the sound transformation through narrow ducts is little affected by one-sided isosurfaces in between. As expected, the beginning of the core region depends on frequency. If the full audio range up to 20 kHz is to be covered, a location in the first bend of the ear canal is found.

[1]  W R Funnell,et al.  On the incorporation of moiré shape measurements in finite-element models of the cat eardrum. , 1996, The Journal of the Acoustical Society of America.

[2]  Christian Weistenhöfer,et al.  Determination of the Shape and Inertia Properties of the Human Auditory Ossicles , 1999, Audiology and Neurotology.

[3]  Sunil Puria,et al.  Finite element modeling of acousto-mechanical coupling in the cat middle ear. , 2008, The Journal of the Acoustical Society of America.

[4]  H. Hudde,et al.  Estimation of the area function of human ear canals by sound pressure measurements. , 1983, The Journal of the Acoustical Society of America.

[5]  S M Khanna,et al.  Sound propagation in the ear canal and coupling to the eardrum, with measurements on model systems. , 1989, The Journal of the Acoustical Society of America.

[6]  R. Rabbitt,et al.  Acoustic intensity, impedance and reflection coefficient in the human ear canal. , 2002, The Journal of the Acoustical Society of America.

[7]  Michael R Stinson,et al.  Comparison of an analytic horn equation approach and a boundary element method for the calculation of sound fields in the human ear canal. , 2005, The Journal of the Acoustical Society of America.

[8]  G A Daigle,et al.  Transverse pressure distributions in a simple model ear canal occluded by a hearing aid test fixture. , 2007, The Journal of the Acoustical Society of America.

[9]  M. R. Stinson,et al.  The spatial distribution of sound pressure within scaled replicas of the human ear canal. , 1985, The Journal of the Acoustical Society of America.

[10]  R D Rabbitt,et al.  Ear canal cross-sectional pressure distributions: mathematical analysis and computation. , 1991, The Journal of the Acoustical Society of America.

[11]  R. Rabbitt,et al.  Three-dimensional acoustic waves in the ear canal and their interaction with the tympanic membrane. , 1988, The Journal of the Acoustical Society of America.

[12]  A G Webster,et al.  Acoustical Impedance and the Theory of Horns and of the Phonograph. , 1919, Proceedings of the National Academy of Sciences of the United States of America.