An electrical tuning mechanism in turtle cochlear hair cells

Abstract

Intracellular recordings were made from single cochlear hair cells in the isolated half-head of the turtle. The electrical responses of the cells were recorded under 2 conditions: when the ear was stimulated with low-intensity tones of different frequencies and when current steps were injected through the intracellular electrode. The extent to which cochlear''s frequency selectivity could be accounted for by the electrical properties of the hair cells, was evaluated. At low levels of acoustic stimulation, the amplitude of the hair cell receptor potential was proportional to sound pressure. The linear tuning curve, which is defined as the sensitivity of the cell as a function of frequency when the cell is operating in its linear range, was measured for a number of hair cells with characteristic frequencies from 86-425 Hz. For small currents the frequency of the oscillations and the quality factor (Q) of the electrical resonance derived from the decay of the oscillations were close to the characteristic frequency and Q of the hair-cell linear tuning curve obtained from sound presentations. The hair cell''s membrane potential change to small-current pulses or low-intensity tone bursts could be largely described by representing the hair cell as a simple electrical resonator consisting of an inductance, resistor and capacitor. When step displacements of 29-250 nm were applied to a micropipette, placed just outside a hair cell in the basilar papilla, an initial periodic firing of impulses could be recorded from single fibers in the auditory nerve. Currents of up to 1 nA, injected through the same micropipette, failed to produce any change in the auditory nerve discharge. Current injection does not produce gross movements of the electrode tip. The contribution of the electrical resonance to hair-cell tuning was assessed by dividing the linear tuning curve by the cell impedance as a function of frequency, assuming that the electrical resonance is independent of other filtering stages; the resonance can thus account for the tip of the acoustical tuning curve. The residual filter exhibited a high-frequency roll-off with a corner frequency at 500-600 Hz, similar in all cells, and a low-frequency roll-off, with a corner frequency from 30 to 350 Hz which varied from cell to cell but was uncorrelated with the characteristic frequency of the cell. The phase of the receptor potential relative to the sound pressure at the tympanum was measured in 10 cells. For low intensities the phase characteristic was independent of sound pressure. At low frequencies the receptor potential led the sound by 270-360.degree., and in the region of the characteristic frequency there was an abrupt phase lag of 90-180.degree.; the abruptness of the phase change depended upon the Q of the cell. The calculated phase shift of the electrical resonator as a function of frequency was subtracted from the phase characteristic of the receptor potential. The subtraction removed the sharp phase transition around the characteristic frequency, and in this frequency region the residual phase after subtraction was approximately constant at + 180.degree.. Hair cells probably depolarize in response to displacements of the basilar membrane towards the scala vestibuli. The high-frequency region of the residual phase characteristic was similar in all cells. Each hair cell contains its own electrical resonance mechanism which accounts for most of the frequency selectivity of the receptor potential. Cells show evidence of a broad band-pass filter, the high frequency portion of which may be produced by the action of the middle ear.