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chapter 36 - Vestibular Mechanics - KEMT FEI TUKE

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everyday movement. Environments such as an aircraft flight can produce frequencies outside the linear<br />

range for these transducers.<br />

Rabbit and Damino [1992] have modeled the flow of endolymph in the ampulla and its interaction<br />

with a cupula. This model indicates that the cupula in the mechanical system appears to add a highfrequency<br />

gain enhancement as well as phase lead over previous mechanical models. This is consistent<br />

with measurements of vestibular nerve recordings of gain and phase. Prior to this work this gain and<br />

phase enhancement were thought to be of hair cell origin.<br />

Defining Terms<br />

Endolymph: Fluid similar to intercellular fluid (high in potassium) which fills the membranous labyrinth,<br />

canals, utricle, and saccule.<br />

Kelvin-Voight viscoelastic material: The simplest of solid materials which have both elastic and viscous<br />

responses of deformation. The viscous and elastic responses appear to act in parallel.<br />

Otolith: Linear accelerometers of the vestibular system whose primary transduced signal is the sum of<br />

linear acceleration and gravity in the frequency range from DC (static) up to the maximum<br />

experienced by an animal.<br />

Semicircular canals: Angular motion sensors of the vestibular system whose primary transduced signal<br />

is angular velocity in the frequency range of normal animal motion.<br />

References<br />

Grant JW, Best WA, Lonegro R. 1984. Governing equations of motion for the otolith organs and their<br />

response to a step change in velocity of the skull. J Biomech Eng 106:203.<br />

Grant JW, Cotton JR. 1991. A model for otolith dynamic response with a viscoelastic gel layer. J <strong>Vestibular</strong><br />

Res 1:139.<br />

Grant JW, Huang CC, Cotton JR. 1994. Theoretical mechanical frequency response of the otolith organs.<br />

J <strong>Vestibular</strong> Res 4(2):137.<br />

Lewis ER, Leverens EL, Bialek WS. 1985. The Vertebrate Inner Ear, Boca Raton, Fla, CRC Press.<br />

Rabbit RD, Damino ER. 1992. A hydroelastic model of macromachanics in the endolymphatic vestibular<br />

canal. J Fluid Mech 238:337.<br />

Van Buskirk WC. 1977. The effects of the utricle on flow in the semicircular canals. Ann Biomed Eng 5:1.<br />

Van Buskirk WC, Grant JW. 1973. Biomechanics of the semicircular canals, pp 53–54, New York, Biomechanics<br />

Symposium of American Society of Mechanical Engineers.<br />

Van Buskirk WC, Grant JW. 1987. <strong>Vestibular</strong> mechanics. In R. Skalak, S. Chien (eds), Handbook of<br />

Bioengineering, pp 31.1–31.17, New York, McGraw-Hill.<br />

Van Buskirk WC, Watts RG, Liu YU. 1976. Fluid mechanics of the semicircular canal. J Fluid Mech 78:87.<br />

Nomenclature<br />

Otolith Variables<br />

x = coordinate direction in the plane of the otoconial layer<br />

y g = coordinate direction normal to the plane of the otolith with origin at the gel base<br />

y f = coordinate direction normal to the plane of the otolith with origin at the fluid base<br />

t = time<br />

u(y f,t) = velocity of the endolymph fluid measured with respect to the skull<br />

v(t) = velocity of the otoconial layer measured with respect to the skull<br />

w(y g,t) = velocity of the gel layer measured with respect to the skull<br />

δ g(y g,t) = displacement of the gel layer measured with respect to the skull<br />

δ o = displacement of the otoconial layer measured with respect to the skull<br />

V s = skull velocity in the x direction measured with respect to an inertial reference frame<br />

V = a characteristic velocity of the skull in the problem (magnitude of a step change)<br />

© 2000 by CRC Press LLC

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