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龟耳蜗毛细胞中的电调谐机制。

An electrical tuning mechanism in turtle cochlear hair cells.

作者信息

Crawford A C, Fettiplace R

出版信息

J Physiol. 1981 Mar;312:377-412. doi: 10.1113/jphysiol.1981.sp013634.

Abstract
  1. 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 two conditions: (a) when the ear was stimulated with low-intensity tones of different frequencies and (b) when current steps were injected through the intracellular electrode. The aim of the experiments was to evaluate the extent to which the cochlea's frequency selectivity could be accounted for by the electrical properties of the hair cells.2. At low levels of acoustic stimulation, the amplitude of the hair cell's 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 Hz to 425 Hz.3. A rectangular current passed into a hair cell elicited a membrane potential change consisting of a damped oscillation superimposed on a step. Small currents produced symmetrical oscillations at the beginning and end of the pulse. Larger currents increased the initial ringing frequency if depolarizing and decreased it if hyperpolarizing.4. 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.5. 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.6. 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 fibres 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. The experiment demonstrates that current injection does not produce gross movements of the electrode tip.7. The contribution of the electrical resonance to hair-cell tuning was assessed by dividing the linear tuning curve by the cell's impedance as a function of frequency. The procedure assumes that the electrical resonance is independent of other filtering stages, and on this assumption the resonance can account for the tip of the acoustical tuning curve.8. The residual filter produced by the division was broad; it 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.9. The phase of the receptor potential relative to the sound pressure at the tympanum was measured in ten cells. For low intensities the phase characteristic was independent of the sound pressure. At low frequencies the receptor potential led the sound by 270-360 degrees , and in the region of the characteristic frequency there was an abrupt phase lag of 90-180 degrees ; the abruptness of the phase change depended upon the Q of the cell.10. 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 degrees . This is consistent with the idea that the hair cells 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.11. It is concluded that each hair cell contains its own electrical resonance mechanism which accounts for most of the frequency selectivity of the receptor potential. All cells also show evidence of a broad band-pass filter, the high frequency portion of which may be produced by the action of the middle ear.
摘要
  1. 在海龟离体半侧头部的单个耳蜗毛细胞上进行细胞内记录。在两种条件下记录细胞的电反应:(a) 用不同频率的低强度纯音刺激耳朵时;(b) 通过细胞内电极注入电流阶跃时。实验目的是评估毛细胞的电特性在多大程度上可以解释耳蜗的频率选择性。

  2. 在低声学刺激水平下,毛细胞感受器电位的幅度与声压成正比。线性调谐曲线定义为细胞在其线性范围内作为频率函数的灵敏度,对多个特征频率在86 Hz至425 Hz之间的毛细胞进行了测量。

  3. 注入毛细胞的矩形电流引起膜电位变化,该变化由叠加在阶跃上的阻尼振荡组成。小电流在脉冲开始和结束时产生对称振荡。较大电流如果是去极化则增加初始振铃频率,如果是超极化则降低初始振铃频率。

  4. 对于小电流,振荡频率和从振荡衰减得出的电共振品质因数(Q)接近从声音刺激获得的毛细胞线性调谐曲线的特征频率和Q。

  5. 毛细胞对小电流脉冲或低强度音爆的膜电位变化在很大程度上可以通过将毛细胞表示为由电感、电阻和电容组成的简单电谐振器来描述。

  6. 当对置于基底乳头中毛细胞外的微电极施加29 - 250 nm的阶跃位移时,可以从听神经的单根纤维记录到初始的周期性冲动发放。通过同一微电极注入高达1 nA的电流未能使听神经放电产生任何变化。该实验表明电流注入不会使电极尖端产生明显移动。

  7. 通过将线性调谐曲线除以细胞作为频率函数的阻抗来评估电共振对毛细胞调谐的贡献。该过程假设电共振独立于其他滤波阶段,基于此假设,共振可以解释声学调谐曲线的尖端。

  8. 除法产生的残余滤波器很宽;它在500 - 600 Hz处呈现高频滚降,所有细胞类似,并且在30至350 Hz处呈现低频滚降,其转折频率因细胞而异,但与细胞的特征频率无关。

  9. 在十个细胞中测量了感受器电位相对于鼓膜处声压的相位。对于低强度,相位特性与声压无关。在低频时,感受器电位超前声压27° - 360°,在特征频率区域存在90° - 180°的突然相位滞后;相位变化的突然程度取决于细胞的Q值。

  10. 从感受器电位的相位特性中减去电谐振器作为频率函数的计算相位偏移。减法消除了特征频率周围的尖锐相位转变,在该频率区域,减法后的残余相位在 +180° 左右近似恒定。这与毛细胞响应基底膜向前庭阶位移而发生去极化的观点一致。所有细胞残余相位特性的高频区域相似。

  11. 得出的结论是,每个毛细胞都包含其自身的电共振机制,该机制解释了感受器电位的大部分频率选择性。所有细胞还显示出宽带通滤波器的证据,其高频部分可能由中耳的作用产生。

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本文引用的文献

1
Ion movements during nerve activity.神经活动期间的离子运动。
Ann N Y Acad Sci. 1959 Aug 28;81:221-46. doi: 10.1111/j.1749-6632.1959.tb49311.x.
4
The origin of tuning in turtle cochlear hair cells.龟类耳蜗毛细胞调谐的起源。
Hear Res. 1980 Jun;2(3-4):447-54. doi: 10.1016/0378-5955(80)90081-7.

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