Titlebook: Auditory Frequency Selectivity; Brian C. J. Moore,Roy D. Patterson Book 1986 Springer Science+Business Media New York 1986 biophysics.fiel

Spinal-Fusion

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HAWK

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Auctions in Theory and Practice,ty is based upon mechanical resonance of individual hair bundles (Frishkopf and DeRosier, 1983; Holton and Hudspeth, 1983). In this instance, such mechanical properties of the bundles as their lengths, masses, drags and stiffnesses determine the characteristic frequencies of the hair cells.

meritorious

Correlation Between the Kinetic Properties of Ionic Channels and the Frequency of Membrane-Potentialty is based upon mechanical resonance of individual hair bundles (Frishkopf and DeRosier, 1983; Holton and Hudspeth, 1983). In this instance, such mechanical properties of the bundles as their lengths, masses, drags and stiffnesses determine the characteristic frequencies of the hair cells.

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Changes in Cochlear Frequency Selectivity Produced by Tectorial-Membrane Manipulation necessary to assume that its system is tightly coupled to the resonance system of the basilar membrane, consisting of the membrane’s stiffness and the mass it supports. In this way a two-resonator system results for every longitudinal element of the cochlear canal.

Flavouring

Asymmetry in Reflection of Cochlear Wavess a distinct asymmetry in reflection of cochlear waves. Reverse waves, travelling towards the stapes, are much more reflected than waves travelling towards the helicotrema. (ii) The decline of the stiffness of the basilar membrane is the principal feature determining the reflection properties.

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incite

Akio Matsumoto,Ferenc Szidarovszky cf’s ranging approximately from 10 Hz to 150 Hz, with substantial sensitivity extending to 200 Hz (Koyama et al., 1980). Afferents from this endorgan exhibit neither adaptation nor two-tone suppression.