OHCs amplify sound by an electromechanical mechanism. Sound-induced vibrations cause OHC membrane potential (E) to change from its resting voltage (Em) to a new value (Em+dE). The induced receptor potential (dE) initiates charge movement (Q) and force production to counteract viscous losses incurred by the traveling wave. Q exhibits a sigmoidal function with E and because it is most sensitive to dE at the midpoint (Vm), Em should equal Vm to ensure maximum amplification. Vm was measured with isolated OHCs extracted from guinea pig with whole-cell patch clamp under constant intracellular pressure in presence of KCNQ4 blocker XE991 (≥ 30 μM) to ensure robust voltage clamp (conductance < 1.5 nS at Vm). After correcting for physiological conditions the results show Vm is coincident with in vitro measurements of Em (Neuron 2011 70: 1143), but a mismatch of 40 mV is apparent when comparing with in vivo measurements of Em made at basal (J. Physiol. 1987 383: 551 and Proc. R. Soc. Lond. B. 1992 247: 97) or apical (J. Neuroscience 1985 5: 1591) regions of cochlea. Results also reveal variation of Vm across the cochlea as a function of a non-uniform charge density of the lateral wall (σ); when σ is uniform Vm is constant, and when σ varies inversely with area of lateral wall (ALW)Vm increases monotonically from a hyperpolarized value at the high frequency region of cochlea to a depolarized value at low frequency region. Although the relationship between Vm and σ is satisfying as it reflects the electric field, the disparity between in vitro and in vivo measurements highlights the need to reconcile them to ascertain the operating position of the amplifier.
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