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S M Novoselova

Publications and source records attributed to S M Novoselova.

4 recordsLinked to original sources

A possibility of sharp tuning in a linear transversally inhomogeneous cochlear model.

Considerable sharpening of basilar membrane frequency selectivity and simultaneous decreasing of phase lag can be obtained in a linear ('passive') hydromechanical three-dimensional cochlear model, if the transverse geometry of the cochlea is taken into account. Both the tuning qualities, Q10, and the phase angles at CF of some transversally inhomogeneous linear models can be set into the range of experimental data [Sellick et al. (1983) Hear. Res. 10, 93-108; Robles et al. (1986) J. Acoust. Soc. Am. 80, 1364-1379.] The calculations are developed on the base of WKB-approximation. The integral coefficients of eiconal equation are the transversally averaged means of basilar membrane surface mass density and stiffness: (formula; see text) where eta(y) is the major eigenfunction of basilar membrane cross-sectional vibrations. The classical Ritz's method is used for calculation of the cross-sectional eigenfunctions. The size and the form of cochlear cross-section are found also to alter the tuning. The rapid increase of the model response towards the peak is due to that damping remains negligible up to the peak position, where the imaginery part of the wave-number begins to increase sharply.

Acoustic Stimulation

[Basilar membrane nonlinearity].

The nonlinear correction of the cochlear partitions movement equation becomes the main part in the resonant section. In the neighbourhood of this section the periodic solution, having the drawing force frequency omega, gets the region of the non-stability in the interval (see abstract), where a is the vibration amplitude and h is the basilar membrane thickness. The amplitude jump in the unstable region may be a stimulus exciting the hair cells and also the cause of cochlear eddies phenomenon.

Basilar Membrane

[Assessment of the anisotropic stiffness component of the basilar membrane].

The average through the section components Dy and Dx of the basilar membrane anisotropic stiffness are evaluated from Bekesy's hydrostatic and hair probe experiments. A contradiction is found between the values and the behaviour of Dy component, calculated from the hydrostatic experiment and from the hair probe. The solution of the strongly bent plate equation for the average through the section transversal component of the basilar membrane anisotropic stiffness is obtained by the asymptotic method. A significant divergence between effective and bending stiffness can exist if the thickness of the human basilar membrane is about twice of that of the guinea pig.

Animals