Turtle Hair Cells Research Articles

Pharmacologically distinct nicotinic acetylcholine receptors drive efferent-mediated excitation in calyx-bearing vestibular afferents.

Electrical stimulation of vestibular efferent neurons rapidly excites the resting discharge of calyx/dimorphic (CD) afferents. In turtle, this excitation arises when acetylcholine (ACh), released from efferent terminals, directly depolarizes calyceal endings by activating nicotinic ACh receptors (nAChRs). Although molecular biological data from the peripheral vestibular system implicate most of the known nAChR subunits, specific information about those contributing to efferent-mediated excitation of CD afferents is lacking. We sought to identify the nAChR subunits that underlie the rapid excitation of CD afferents and whether they differ from α9α10 nAChRs on type II hair cells that drive efferent-mediated inhibition in adjacent bouton afferents. We recorded from CD and bouton afferents innervating the turtle posterior crista during electrical stimulation of vestibular efferents while applying several subtype-selective nAChR agonists and antagonists. The α9α10 nAChR antagonists, α-bungarotoxin and α-conotoxin RgIA, blocked efferent-mediated inhibition in bouton afferents while leaving efferent-mediated excitation in CD units largely intact. Conversely, 5-iodo-A-85380, sazetidine-A, varenicline, α-conotoxin MII, and bPiDDB (N,N-dodecane-1,12-diyl-bis-3-picolinium dibromide) blocked efferent-mediated excitation in CD afferents without affecting efferent-mediated inhibition in bouton afferents. This pharmacological profile suggested that calyceal nAChRs contain α6 and β2, but not α9, nAChR subunits. Selective blockade of efferent-mediated excitation in CD afferents distinguished dimorphic from calyx afferents by revealing type II hair cell input. Dimorphic afferents differed in having higher mean discharge rates and a mean efferent-mediated excitation that was smaller in amplitude yet longer in duration. Molecular biological data demonstrated the expression of α9 in turtle hair cells and α4 and β2 in associated vestibular ganglia.

Gating of Two Mechanoelectrical Transducer Channels Associated with a Single Tip Link

Although gating of mechanoelectrical transducer (MET) channels has been successfully described by assuming that one channel is associated with a tip link in the hair bundle, recent reports indicate that a single tip link is associated with more than one channel. To address the consistency of the model with the observations, gating of MET channels is described here by assuming that each tip link is associated with two identical MET channels, which are connected either in series or in parallel. We found that series connection does not lead to a single minimum of stiffness with respect to hair bundle displacement unless the minimum is above a certain positive value. Thus, negative stiffness must appear in pairs in the displacement axis. In contrast, parallel connection of the two channels predicts gating compliance similar to that predicted by the one-channel-per-tip-link model of channel gating, within the physiological range of parameters. Parallel connection of MET channels is, therefore, a reasonable assumption to explain most experimental observations. However, the compatibility with series connection cannot be ruled out for experimental data on turtle hair cells.

Effects of phenylalkylamines and benzothiazepines on Cav1.3-mediated Ca2+ currents in neonatal mouse inner hair cells

Calcium currents (I(Ca)) in inner hair cells (IHCs) are carried by the Ca(v)1.3 subtype of L-type calcium channels. They play an important role in synaptic transmission of sound-evoked mechanical stimuli. L-type calcium channels are targets of the organic blocker classes dihydropyridines, phenylalkylamines and benzothiazepines. Previously a low sensitivity of the Ca(v)1.3 subtype towards dihydropyridines has been demonstrated. Therefore, this study evaluates the effect of two phenylalkylamines (verapamil and gallopamil) and the benzothiazepine diltiazem on I(Ca) through Ca(v)1.3 channels in mouse IHCs. Whole-cell I(Ca) was measured using the patch-clamp technique in mouse IHCs aged postnatal day 3-7 with 5 mM calcium as a charge carrier. The phenylalkylamines verapamil and gallopamil and the benzothiazepine diltiazem inhibited I(Ca) in IHCs in a concentration-dependent manner. This block was largely reversible. Dose-response curves revealed IC(50) values of 199+/-19 microM for verapamil, 466+/-151 microM for gallopamil and 326+/-67 microM for diltiazem. The inhibition of peak I(Ca) by phenylalkylamines and benzothiazepines was voltage-independent. Verapamil (300 microM) enhanced current inactivation from -20 to +20 mV while diltiazem (300 microM) did so only at very depolarised potentials (+20 mV). In conclusion, the concentrations of phenylalkylamines and benzothiazepine necessary to inhibit 50% of I(Ca) in IHCs were one order larger compared to concentrations which inhibited I(Ca) through Ca(v)1.2 channels in native cells or expression systems. However, inhibitory concentrations were in the same range as those required for block of I(Ca) in turtle hair cells.

Quantitative analysis of stereociliary arrays on vestibular hair cells

We have developed a method for quantifying the number, spacing, and distribution of stereocilia on the apical surface of hair cells using spatial autocorrelation analysis and statistics for directional data. Here, we illustrate the method using idealized hair bundles, and we apply it to scanning micrographs of turtle hair cells from the utricle and posterior canal, and to freeze-fracture preparations of bullfrog saccule. The analysis suggests three common features of stereociliary bundles. First, bundle geometries form a continuum from ‘loose’ to ‘tight’ (Acta Otolaryngol. 106 (1988) 393) rather than two distinct groups. Second, interciliary spacing along the three hexagon axes is not equal; spacing is usually widest along the hexagon axis closest to the bundle’s axis of bilateral symmetry (the presumptive excitatory axis). Third, spacing between stereocilia changes with distance from the kinocilium. All three features will influence predictions of the tip link tensions that accompany bundle deflection.

Fast adaptation of mechanoelectrical transducer channels in mammalian cochlear hair cells.

Outer hair cells are centrally involved in the amplification and frequency tuning of the mammalian cochlea, but evidence about their transducing properties in animals with fully developed hearing is lacking. Here we describe measurements of mechanoelectrical transducer currents in outer hair cells of rats between postnatal days 5 and 18, before and after the onset of hearing. Deflection of hair bundles using a new rapid piezoelectric stimulator evoked transducer currents with ultra-fast activation and adaptation kinetics. Fast adaptation resembled the same process in turtle hair cells, where it is regulated by changes in stereociliary calcium. It is argued that sub-millisecond transducer adaptation can operate in outer hair cells under the ionic, driving force and temperature conditions that prevail in the intact mammalian cochlea.

The Distribution of Calcium Buffering Proteins in the Turtle Cochlea

Hair cells of the inner ear contain high concentrations of calcium-binding proteins that limit calcium signals and prevent cross talk between different signaling pathways during auditory transduction. Using light microscope immunofluorescence and post-embedding immunogold labeling in the electron microscope, we characterized the distribution of three calcium-buffering proteins in the turtle cochlea. Both calbindin-D28k and parvalbumin-beta were confined to hair cells in which they showed a similar distribution, whereas calretinin was present mainly in hair-cell nuclei but also occurred in supporting cells and nerve fibers. The hair-cell concentration of calbindin-D28k but not of parvalbumin-beta increased from the low- to high-frequency end of the cochlea. Calibration against standards containing known amounts of calcium-buffering protein processed in the same fluid drop as the cochlear sections gave cytoplasmic concentrations of calbindin-D28k as 0.13-0.63 mm and parvalbumin-beta as approximately 0.25 mm, but calretinin was an order of magnitude less. Total amount of Ca 2+-binding sites on the proteins is at least 1.0 mm in low-frequency hair cells and 3.0 mm in high-frequency cells. Reverse transcription-PCR showed that mRNA for all three proteins was expressed in turtle hair cells. We suggest that calbindin-D28k and parvalbumin-beta may serve as endogenous mobile calcium buffers, but the predominantly nuclear location of calretinin argues for another role in calcium signaling. The results support conclusions from electrophysiological measurements that millimolar concentrations of endogenous calcium buffers are present in turtle hair cells. Parvalbumin-beta was also found in both inner and outer hair cells of the guinea pig cochlea.

Active Hair Bundle Motion Linked to Fast Transducer Adaptation in Auditory Hair Cells

During transduction in auditory hair cells, hair bundle deflection opens mechanotransducer channels that subsequently reclose or adapt to maintained stimuli, a major component of the adaptation occurring on a submillisecond time scale. Using a photodiode imaging technique, we measured hair bundle motion in voltage-clamped turtle hair cells to search for a mechanical correlate of fast adaptation. Excitatory force steps imposed by a flexible glass fiber attached to the bundle caused an initial movement toward the kinocilium, followed by a fast recoil equivalent to bundle stiffening. The recoil had a time course identical to adaptation of the transducer current, and like adaptation, was most prominent for small stimuli, was slowed by reducing extracellular calcium, and varied with hair cell resonant frequency. In free-standing hair bundles, depolarizations positive to 0 mV evoked an outward current attributable to opening of transducer channels, which was accompanied by a sustained bundle deflection toward the kinocilium. Both processes were sensitive to external calcium concentration and were abolished by blocking the transducer channels with dihydrostreptomycin. The similarity in properties of fast adaptation and the associated bundle motion indicates the operation of a rapid calcium-sensitive force generator linked to the gating of the transducer channels. This force generator may permit stimulus amplification during transduction in auditory hair cells.

The functional role of alternative splicing of Ca(2+)-activated K+ channels in auditory hair cells.

Turtle auditory hair cells are frequency tuned by the activity of large-conductance calcium-activated potassium (KCa) channels, the frequency range being dictated primarily by the channel kinetics. Seven alternatively spliced isoforms of the KCa channel alpha-subunit, resulting from exon insertion at two splice sites, were isolated from turtle hair cells. These, when expressed in Xenopus oocytes, produced KCa channels with a range of apparent calcium sensitivities and channel kinetics. However, most expressed channels were less calcium sensitive than the hair cells' native KCa channels. Coexpression of alpha-subunit with a bovine beta-subunit substantially increased the channel's calcium sensitivity while markedly slowing its kinetics, but kinetic differences between isoforms were preserved. These data suggest a molecular mechanism for hair cell frequency tuning involving differential expression of different KCa channel alpha-subunits in conjunction with an expression gradient of a regulatory beta-subunit.

The paradox of hair cell adaptation.

The paradox of hair cell adaptation.

Variations in the ensemble of potassium currents underlying resonance in turtle hair cells.

1. Potassium currents were characterized in turtle cochlear hair cells by whole-cell voltage clamp during superfusion with the potassium channel antagonists, tetraethylammonium (TEA) and 4-aminopyridine (4-AP). The estimated resonant frequency, f0, was inferred from tau, the time constant of deactivation of outward current upon repolarization to -50 mV, according to the empirical relation, f0 = k1 tau-1/2 + k2. 2. Dose-response relations for TEA and 4-AP were obtained by exposing single cells to ten concentrations exponentially distributed over four orders of magnitude. Potassium current in cells tuned to low frequencies was carried by a single class of channels with an apparent affinity constant, K1, for TEA of 35.9 mM. Half-blocking concentrations of 4-AP were correlated with the time constant of deactivation and varied between 26.2 and 102 microM. In cells tuned to higher frequencies, K+ current was carried by a single class of channels with high affinity for TEA (K1 = 0.215 mM) and low affinity for 4-AP (K1 = 12.3 mM). This pharmacological profile suggests that K+ current in low frequency cells is purely voltage gated and in high frequency cells, it is gated by both Ca2+ and voltage. 3. For each current type, the voltage dependence of activation was determined from tail current amplitude at -50 mV. The purely voltage-gated current, IK(V), was found to increase e-fold in 4.0 +/- 0.3 mV (n = 3) in low frequency cells exposed to TEA (25 mM). The Ca(2+)- and voltage-gated current, IK(Ca), was more steeply voltage dependent, increasing e-fold in 1.9 mV (n = 2) in high frequency cells exposed to 4-AP (0.8 mM). 4. IK(V) was found to inactivate slowly during prolonged voltage steps (approximately 10 s). Steady-state inactivation increased with depolarization from -70 mV and was incomplete such that on average IK(v) did not fall below approximately 0.39 of its maximum value. 5. Superfusion of 4-AP (0.8 mM) reversibly depolarized a low frequency cell and eliminated steady voltage oscillations, while TEA (6 mM) had no effect. In a high frequency cell, voltage oscillations were abolished by TEA, but not by 4-AP. 6. The differential pharmacology of IK(V) and IK(Ca) was used to measure their contribution to K+ current in cells tuned to different frequencies. Both currents exhibited a frequency-dependent increase in maximum conductance. IK(V) accounted for nearly all K+ current in cells tuned to less than 60 Hz, while IK(Ca) was the dominant current in higher frequency cells. 7. Mapping resonant frequency onto epithelial position suggests an exponential relation between K+ current size and position. IK(V) appeared to be limited to the apical or low frequency portion of the basilar papilla and coincided with maximal expression of a K(+)-selective inward rectifier, IK(IR). This finding is consistent with the notion that low frequency resonance is produced by interaction of IK(V) and IK(IR) with the voltage-gated Ca2+ current, ICa, and the cell's capacitance. The ionic events underlying higher frequency resonance are dominated by the action of IK(Ca) and ICa and include a contribution from IK(IR).

A theoretical study of calcium microdomains in turtle hair cells

Confocal imaging has revealed microdomains of intracellular free Ca2+ in turtle hair cells evoked by depolarizing pulses and has delineated factors affecting the growth and dissipation of such domains. However, imaging experiments have limited spatial and temporal resolution. To extend the range of the results we have developed a three-dimensional model of Ca2+ diffusion in a cylindrical hair cell, allowing part of the Ca2+ influx to occur over a small circular region (radius 0.125-1.0 micron) representing a high-density array of voltage-dependent channels. The model incorporated experimental information about the number of channels, the fixed and mobile Ca2+ buffers, and the Ca2+ extrusion mechanism. A feature of the calculations was the use of a variable grid size depending on the proximity to the Ca2+ channel cluster. The results agreed qualitatively with experimental data on the localization of the Ca2+ transients, although the experimental responses were smaller and slower, which is most likely due to temporal and spatial averaging in the imaging. The model made predictions about 1) the optimal Ca2+ channel number and density within a cluster, 2) the conditions to ensure independence of neighboring clusters, and 3) the influence of the Ca2+ buffers on the kinetics and localization of the microdomains. We suggest that an increase in the mobile Ca2+ buffer concentration in high-frequency hair cells (which possess a larger number of release sites) would allow lower amplitude and faster Ca2+ responses and promote functional independence of the sites.

Monitoring calcium in turtle hair cells with a calcium-activated potassium channel.

1. An apamin-sensitive Ca(2+)-activated K+ channel was characterized in turtle hair cells and utilized to monitor submembranous intracellular Ca2+ and to evaluate the concentration of the mobile endogenous calcium buffer. 2. Isolated hair cells were voltage clamped with whole-cell patch electrodes filled with a Cs(+)-based intracellular solution to block the large-conductance Ca(2+)-activated K+ (BK) channel. Ca2+ currents evoked by depolarization were followed by inward tail currents lasting several hundred milliseconds. Both the Ca2+ current and slow tail current were abolished by nifedipine. 3. The tail current was carried by K+ and Cs+ (relative permeabilities PCa/PK = 0.22), and was fully blocked by 0.1 microM apamin and half blocked by 5 mM external TEA. These properties suggest the tail current flows through a Ca(2+)-activated K+ channel distinct from the BK channels. 4. Intracellular Ca2+ was imaged with a confocal microscope in hair cells filled with the indicator Calcium Green-5N introduced via the patch pipette. Increases in Ca2+ evoked by depolarization were localized to hotspots on the basolateral surface of the cell. The time course of the tail current closely matched the fast component of the fluorescenece monitored at a hotspot. 5. Ca(2+)-ATPase pump inhibitors thapsigargin, 2,4-di-(t-butyl)hydroquinone (BHQ) and vanadate, which are known to influence calcium regulation in turtle hair cells, prolonged the time course of the tail current, supporting the idea that the channel monitors cytoplasmic Ca2+. 6. The mobile endogenous buffer was estimated by combining perforated-patch and whole-cell recordings on a single cell. After recording tail currents with an amphotericin-perforated patch, the patch was ruptured to obtain the whole-cell mode, thus allowing washout of soluble cytoplasmic proteins and exchange with pipette buffers. By varying the concentration of Ca2+ buffer in the pipette, the mobile endogenous buffer was found to be equivalent to about 1 mM BAPTA.

Routes of calcium entry and extrusion in turtle hair cells.

Routes of calcium entry and extrusion in turtle hair cells.

A developmental model for generating frequency maps in the reptilian and avian cochleas

Hair cells in the turtle cochlea are frequency-tuned by a mechanism involving the combined activation of voltage-sensitive Ca2+ channels and Ca(2+)-activated K+ (KCa) channels. The main determinants of a hair cell's characteristic frequency (Fo) are the KCa channels' density and kinetics, both of which change systematically with location in the cochlea in conjunction with the observed frequency map. We have developed a model based on the differential expression of two KCa channel subunits, which when accompanied by concurrent changes in other properties (e.g., density of Ca2+ channels and inwardly rectifying K+ channels), will generate sharp tuning at frequencies from 40 to 600 Hz. The kinetic properties of the two subunits were derived from previous single-channel analysis, and it was assumed that the subunits (A and B) combine to form five species of tetrameric channel (A4, A3B, A2B2, AB3, and B4) with intermediate kinetics and overlapping distribution. Expression of KCa and other channels was assumed to be regulated by diffusional gradients in either one or two chemicals. The results are consistent with both current- and voltage-clamp data on turtle hair cells, and they show that five channel species are sufficient to produce smooth changes in both Fo and kinetics of the macroscopic KCa current. Other schemes for varying KCa channel kinetics are examined, including one that allows extension of the model to the chick cochlea to produce hair cells with Fo's from 130 to 4000 Hz. A necessary assumption in all models is a gradient in the values of the parameters identified with the cell's cytoplasmic Ca2+ buffer.

Confocal imaging of calcium microdomains and calcium extrusion in turtle hair cells

We have studied spatial Ca2+ distribution in hair cells filled with the low affinity fluorescent indicator Calcium Green 5N using real-time confocal microscopy and whole-cell recording. During depolarizations lasting several hundred milliseconds, Ca2+ fluorescence increased at a number of hotspots around the base of the cell but changed little near the hair bundle. The hotspots required influx of Ca2+ through voltage-dependent channels, and they expanded during the pulse from an initial diameter of < 1 pm. Strong Ca2+ buffers like BAPTA slowed their growth rate. On repolarization, the fluorescence decayed with two time constants: ∼ 0.1 s, which may represent Ca2+ diffusion away from the entry sites, and 10 s, probably reflecting Ca2+ extrusion. Extrusion occurs mainly via a CaATPase that can be blocked by vanadate. We suggest the hotspots are m icrodomains of Ca2+ attaining a concentration of at least 85 μM near assemblies of synaptic release sites.

The calcium-activated potassium channels of turtle hair cells.

A major factor determining the electrical resonant frequency of turtle cochlear hair cells is the time course of the Ca-activated K current (Art, J. J., and R. Fettiplace. 1987. Journal of Physiology. 385:207-242). We have examined the notion that this time course is dictated by the K channel kinetics by recording single Ca-activated K channels in inside-out patches from isolated cells. A hair cell's resonant frequency was estimated from its known correlation with the dimensions of the hair bundle. All cells possess BK channels with a similar unit conductance of approximately 320 pS but with different mean open times of 0.25-12 ms. The time constant of relaxation of the average single-channel current at -50 mV in 4 microM Ca varied between cells from 0.4 to 13 ms and was correlated with the hair bundle height. The magnitude and voltage dependence of the time constant agree with the expected behavior of the macroscopic K(Ca) current, whose speed may thus be limited by the channel kinetics. All BK channels had similar sensitivities to Ca which produced half-maximal activation for a concentration of approximately 2 microM at +50 mV and 12 microM at -50 mV. We estimate from the voltage dependence of the whole-cell K(Ca) current that the BK channels may be fully activated at -35 mV by a rise in intracellular Ca to 50 microM. BK channels were occasionally observed to switch between slow and fast gating modes which raises the possibility that the range of kinetics of BK channels observed in different hair cells reflects a common channel protein whose kinetics are regulated by an unidentified intracellular factor. Membrane patches also contained 30 pS SK channels which were approximately 5 times more Ca-sensitive than BK channels at -50 mV. The SK channels may underlie the inhibitory synaptic potential produced in hair cells by efferent stimulation.

The effects of low calcium on the voltage-dependent conductances involved in tuning of turtle hair cells.

1. The voltage-dependent conductances of turtle cochlear hair cells of known resonant frequency were characterized by tight-seal, whole-cell recording during superfusion with solutions containing normal (2.8 mM) and reduced (0.1-10 microM) Ca2+. 2. In 1 microM Ca2+, the current flowing through the voltage-dependent Ca2+ channels was increased roughly fivefold and had a reversal potential near 0 mV. This observation may be explained by the Ca2+ channels becoming non-selectively permeable to monovalent cations in low-Ca2+ solutions. Lowering the Ca2+ further to 0.1 microM produced little increase in the current. 3. The size of the non-selective current increased systematically with the resonant frequency of the hair cell over the range from 10 to 320 Hz. This suggests that hair cells tuned to higher frequencies contain more voltage-dependent Ca2+ channels. 4. There was a good correlation between the amplitudes of the non-selective current and the K+ current which underlies electrical tuning of these hair cells. The amplitude of the K+ current also increased systematically with resonant frequency. 5. In cells with resonant frequencies between 120 and 320 Hz, the K+ current was completely abolished in 1 microM Ca2+, consistent with prior evidence that this current flows through Ca2+ activated K+ channels. In a majority of cells tuned between 50 and 120 Hz, the K+ current was incompletely blocked in 1 microM Ca2+, but was eliminated in 0.1 microM Ca2+. In all hair cells the K+ current was abolished by 25 mM tetraethylammonium chloride. 6. In cells tuned to 10-20 Hz, the K+ current was not substantially diminished even in 0.1 microM Ca2+, which argues that it may not be Ca2+ activated. 7. In cells tuned to frequencies above 100 Hz, the K+ current could still be evoked by depolarization during superfusion with 10 microM Ca2+. However, its half-activation voltage was shifted to more depolarized levels and its maximum amplitude was systematically reduced with increasing resonant frequency. 8. These observations are consistent with the notion that in cells tuned to more than 50 Hz, there is a fixed ratio of the number of voltage-dependent Ca2+ channels to Ca(2+)-activated K+ channels, the numbers of each increasing in proportion to resonant frequency. The results also provide indirect evidence that the Ca(2+)-activated K+ channels in cells tuned to higher frequencies may be less sensitive to intracellular Ca2+.

The actions of calcium on the mechano‐electrical transducer current of turtle hair cells.

1. Mechano-electrical transducer currents evoked by deflections of the hair bundle were recorded in turtle isolated hair cells under whole-cell voltage clamp. The outcome of perfusing with solutions of reduced Ca2+ concentration was investigated. 2. The transducer current was roughly doubled by lowering the concentration of divalent cations from normal (2.2 mM-Mg2+, 2.8 mM-Ca2+) to 0 Mg2+, 0.5 mM-Ca2+. No significant effects on the current's kinetics or reversal potential, or on the current-displacement relationship, were noted. 3. If the Ca2+ concentration was lowered to 50 microM (with no Mg2+), there was about a threefold increase in the maximum current but other changes, including loss of adaptation and a decreased slope and negative shift in the current-displacement relationship, were also observed. As a result, more than half the peak transducer current became activated at the resting position of the hair bundle compared to about a tenth in the control solution. 4. The extra changes manifest during perfusion with 50 microM-Ca2+ had also been seen when the cell was held at positive potentials near the Ca2+ equilibrium potential. This supports the view that some consequences of reduced external Ca2+ stem from a decline in its intracellular concentration. 5. With 20 microM-Ca2+, a standing inward current developed and the cell became unresponsive to mechanical stimuli, which may be explained by the transducer channels being fully activated at the resting position of the bundle. 6. The results are interpreted in terms of a dual action of Ca2+: an external block of the transducer channel which reduces the maximum current, and an intracellular effect on the position and slope of the current-displacement relationship; the latter effect can be modelled by internal Ca2+ stabilizing one of the closed states of the channel. 7. During perfusion with 1 microM-Ca2+, the holding current transiently increased but then returned to near its control level. There was a concomitant irreversible loss of sensitivity to hair bundle displacements which we suggest is due to rupture of the mechanical linkages to the transducer channel. 8. Following treatment with 1 microM-Ca2+, single-channel currents with an amplitude of -9 pA at -85 mV were sometimes visible in the whole-cell recording. The probability of such channels being open could be modulated by small deflections of the hair bundle which indicates that they may be the mechano-electrical transducer channels or conductance about 100 pS. 9. Open- and closed-time distributions for the channel were fitted by single exponentials, the mean open time at rest being approximately 1 ms. The mean open time was increased and the mean closed time decreased for movements of the hair bundle towards the kinocilium.(ABSTRACT TRUNCATED AT 400 WORDS)

Activation and adaptation of transducer currents in turtle hair cells.

1. Transducer currents were recorded in turtle cochlear hair cells during mechanical stimulation of the hair bundle. The currents were measured under whole-cell voltage clamp in isolated cells that were firmly stuck to the floor of the recording chamber. 2. Stimuli were calibrated by projecting the image of the hair bundle onto a rapidly scanned 128 photodiode array. This technique showed that, while the cell body was immobilized, the tip of the bundle would follow faithfully the motion of an attached glass probe up to frequencies of more than 1 kHz. 3. The relationship between inward transducer current and bundle displacement was sigmoidal. Maximum currents of 200-400 pA were observed for deflections of the tip of the bundle of 0.5 microns, equivalent to rotating the bundle by about 5 deg. 4. In response to a step deflection of the bundle, the current developed with a time constant (about 0.4 ms for small stimuli) that decreased with the size of displacement. This suggests that the onset of the current was limited by the gating kinetics of the transduction channel. The onset time course was slowed about fourfold for a 20 degrees C drop in temperature. 5. For small maintained displacements, the current relaxed to about a quarter of the peak level with a time constant of 3-5 ms. This adaptation was associated with a shift of the current-displacement relationship in the direction of the stimulus. The rate and extent of adaptation were decreased by lowering external Ca2+. 6. Adaptation was strongly voltage sensitive, and was abolished at holding potentials positive to the reversal potential of the transducer current of about 0 mV. It was also diminished by loading cells with 10 mM of the Ca2+ chelator BAPTA. These observations suggest that adaptation may be partly controlled by influx of Ca2+ through the transducer channels. 7. Removal of adaptation produced asymmetric responses, with fast onsets but slow decays following return of the bundle to its resting position; the offset time course depended on both the magnitude and duration of the prior displacement. 8. In some experiments, hair bundles were deflected with a flexible glass fibre whose motion was monitored using a dual photodiode arrangement. Positive holding potentials abolished adaptation of the transducer currents, but had no influence on the time course of motion of the fibre. We have no evidence therefore that adaptation is caused by a mechanical reorganization within the bundle.

The frequency limits to transduction in hair cells of the turtle cochlea

During transduction in auditory hair cells, displacements of the hair bundle modulate an inward transducer current; this then evokes a receptor potential that is filtered by the electrical properties of the cell membrane. The frequency characteristics of these steps have been studied by recording membrane currents in isolated turtle hair cells. When the hair bundle is rapidly deflected, the transducer current is activated with a maximum time constant of about 0.1 to 0.2 ms at 23 °C, thus faithfully encoding frequencies below 1 kHz. The ensuing receptor potentials are shaped by a sharply tuned resonance resulting from the interaction of a voltage-dependent Ca2+ current and a Ca2+-activated K+ current. The activation time constant for the K+ current varies inversely with, and largely determines, the resonant frequency of the hair cell in the range 20 to 600 Hz. The time constant of the Ca2+ current (0.3 ms) is rapid compared to the K+ current but must impose a corner frequency of about 500 Hz on transmission across the afferent synapse.