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. 1999 Dec 7;96(25):14306–14311. doi: 10.1073/pnas.96.25.14306

Figure 2.

Figure 2

Analysis of a typical response to mechanical stimulation of an active hair bundle. (A) The fiber’s base motion, XB(t), reflected ±10-nm sinusoidal stimulation at 9 Hz, a frequency below the cell’s characteristic frequency of 14 Hz. (B) The fiber’s tip motion, X(t), was more than double the magnitude of stimulation and exhibited a phase lead. (C) The viscous drag force, FD(t), continuously opposed hair-bundle motion. (D) Because viscous dissipation continuously withdrew energy from the hair bundle, the instantaneous viscous-drag power, PD(t), was negative. (E) The elastic force exerted by the stimulus fiber on the hair bundle, FSF(t), was dominated by the bundle’s elastic reactance. (F) The power provided by the stimulus fiber, PSF(t), was greatest during the fast components of the fiber’s tip motion. The fiber resisted negatively directed hair-bundle movement but powered motion in the opposite direction. Each record, the average of 21 cycles of oscillation, has been duplicated to emphasize its periodic features; the vertical lines facilitate comparison of response phases.