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波动分析揭示的青蛙运动和感觉神经纤维中钾通道的差异。

Differences between K channels in motor and sensory nerve fibres of the frog as revealed by fluctuation analysis.

作者信息

Neumcke B, Schwarz W, Stämpfli R

出版信息

Pflugers Arch. 1980 Aug;387(1):9-16. doi: 10.1007/BF00580838.

Abstract

Differences between K channels in the nodal membrane of sensory and motor myelinated nerve fibres of the frog were investigated by fluctuation analysis. Spectral densities, S(f), between 3 Hz and 5 kHz were determined from K-current fluctuations measured between 145 and 460 ms after the onset of depolarizations V between 16 and 80 mV. Fits by the sum of a 1/f component and Lorentzian spectra corresponding to Hodgkin-Huxley n4-kinetics gave significant deviations from the measured spectra. The best fit was obtained by: S(f) = S1/[1+(f/fc)1.5]+S2. The first term can be interpreted as a diffusion spectrum which would originate from gating of K channels governed by an electrodiffusion process. To describe the spectral density at frequencies above 1 kHz it was necessary to add the plateau S2. Time constants taun* = 1/(2pifc) are roughly equal to the conventional Hodgkin-Huxley time constant taun only for pulses V < 40mV. At higher depolarizations taun increases with increasing depolarization in contrast to taun. The variance, var, of conductance fluctuations was determined by integration of the first component of S(f). From var, the probability of the open channel state, and the steady-state K current the single-channel conductance gamma and the number N of K channels per node were calculated; all parameters were corrected for K accumulation during depolarizing pulses. gamma and N were found to be only weakly voltage-dependent. The mean values over all voltages are for motor fibres: gamma=2.7 pS, N = 5.7 x 10(4), and for sensory fibres: gamma = 4.6 pS, N = 5.2 x 10(4). The results suggest two different kinds of K channels in motor and sensory nerve fibres.

摘要

通过涨落分析研究了青蛙有髓感觉神经纤维和运动神经纤维节点膜中钾通道的差异。在16至80 mV的去极化V开始后145至460 ms之间测量钾电流涨落,从而确定3 Hz至5 kHz之间的功率谱密度S(f)。用对应于霍奇金-赫胥黎n4动力学的1/f分量和洛伦兹谱之和进行拟合,结果与实测谱有显著偏差。最佳拟合为:S(f)=S1/[1+(f/fc)^1.5]+S2。第一项可解释为扩散谱,它可能源于由电扩散过程控制的钾通道门控。为了描述高于1 kHz频率处的功率谱密度,有必要加上平台期S2。时间常数taun* = 1/(2πfc)仅在脉冲V < 40 mV时大致等于传统的霍奇金-赫胥黎时间常数taun。在更高的去极化情况下,与taun不同,taun*随去极化增加而增加。通过对S(f)的第一分量进行积分来确定电导涨落的方差var。根据var、开放通道状态的概率和稳态钾电流,计算单通道电导γ和每个节点的钾通道数量N;所有参数都针对去极化脉冲期间的钾积累进行了校正。发现γ和N仅具有微弱的电压依赖性。所有电压下的平均值对于运动纤维为:γ = 2.7 pS,N = 5.7×10^4;对于感觉纤维为:γ = 4.6 pS,N = 5.2×10^4。结果表明运动神经纤维和感觉神经纤维中存在两种不同类型的钾通道。

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