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. 2018 Dec 19;121(3):732–755. doi: 10.1152/jn.00708.2018

Fig. 4.

Fig. 4.

Semicircular canal macromechanics. A and B: rigid labyrinth model prediction for transient cupula volume displacement in response to a step excitatory increase in angular velocity (c.f. Fig. 3C) and for sustained cupula volume displacement in response to a step angular acceleration. C: bode plots showing cupula volume displacement gain and phase as a function of frequency for sinusoidal oscillation of the head. Left axes show magnitude and phase relative to angular head velocity (flat gain above ωL), while right axes are relative to angular head acceleration (flat gain below ωL). D and E: pressure and endolymph displacement as a function of position in the horizontal canal membranous duct for sinusoidal rotation at 0.003 Hz (D) and at 1 Hz (E) (yellow: max; red: zero; and black: min). F: membranous duct deformability alters the high-frequency cupula displacement (thick black) relative to a perfectly rigid canal (gray). Deformability increases the bandwidth (BW) by shifting ωU up and increases high-frequency sensitivity through the role of perilymph deforming the canal. [DF: adapted from Iversen and Rabbitt (2017).]