Molecular aspects of electrical excitation in lipid bilayers and cell membranes.

P Mueller
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Abstract

Several compounds of fungal or bacterial origin (EIM, alamethicin, monazomycin, DJ400B) can be incorporated into planar lipid bilayers where they form molecular channels and generate voltage-dependent ion conductances. When studied by voltage clamp, the kinetic and steady-state characteristics of these conductance changes are in every respect identical to those found in excitable cell membranes, and their major aspects can be quantitatively described by the Hodgkin-Huxley equations. Thus, the steady-state conductance is an expotential function of the membrane potential, the conductance rises with a sigmoid time course and decays exponentially, and the time constants of the conductance changes go through a maximum as a function of the potential. The conductances also show inactivation as seen in the sodium channels of nerve and the potassium channels of muscle. In addition, there appear for particular pulsing sequences certain kinetic transients that cannot be accounted for by the Hodgkin-Huxley equations but are also seen in identical form in nerve. Because the kinetics are identical in all excitable cell membranes and in these bilayers, it is likely that, in spite of the diverse chemical nature of the channel-forming molecules in the bilayers and the widely differing ion selectivities in the cellular systems, the mechanism by which the membrane opens and closes for the flow of ions is essentially the same in all cases. The kinetic data imply that a cooperative process is involved in the gating action. In principle, two different concepts could account for the kinetics--one involving an intramolecular configurational change within a complex permanent channel, the other, the assembly of a channel through the voltage-dependent aggregation of monomeric channel precursors. In the bilayers the high-order dependence of the steady-state conductance and of the gating time constants on the concentration of the channel formers suggests an aggregation mechanism in which the gating involves the voltage-induced insertion of all or part of the channel-forming molecules from the membrane surface into the hydrocarbon region and their subsequent aggregation into open channels by lateral diffusion. The mathematical description of this two-step insertion-aggregation mechanism accounts quantitatively for the entire conductancb-voltage kinetics including inactivation and other kinetic features which deviate from the Hodgkin-Huxley kinetics in the sense that the rate constants of the changes are dependent not only on the membrane potential but also on the value of the conductance and on time. The proposed mechanism is also in agreement with single-channel data for alamethicin which suggest that both the insertion and the aggregation rate constants are voltage-dependent...

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脂质双分子层和细胞膜电激发的分子方面。
几种真菌或细菌来源的化合物(EIM, alamethicin, monazomycin, DJ400B)可以结合到平面脂质双分子层中,在那里它们形成分子通道并产生电压依赖的离子电导。当用电压钳研究时,这些电导变化的动力学和稳态特性在各个方面都与在可兴奋细胞膜中发现的特性相同,它们的主要方面可以用霍奇金-赫胥黎方程定量描述。因此,稳态电导率是膜电位的出势函数,电导率随时间进程呈s型上升,呈指数衰减,电导率变化的时间常数随电位的变化达到最大值。神经钠通道和肌肉钾通道的传导也表现为失活。此外,对于特定的脉冲序列,出现了某些不能用霍奇金-赫胥黎方程解释的动力学瞬态,但在神经中也以相同的形式出现。因为在所有可兴奋的细胞膜和这些双层中,动力学是相同的,所以很可能,尽管双层中通道形成分子的化学性质不同,细胞系统中离子选择性也有很大差异,但在所有情况下,膜为离子流动打开和关闭的机制基本上是相同的。动力学数据表明,浇注过程涉及一个协同过程。原则上,两个不同的概念可以解释动力学——一个涉及复杂永久通道内的分子内构型变化,另一个涉及通过单体通道前体的电压依赖性聚集的通道组装。在双分子层中,稳态电导和门控时间常数对形成通道的分子浓度的高阶依赖性表明了一种聚集机制,其中门控包括电压诱导的全部或部分形成通道的分子从膜表面插入到碳氢化合物区域,然后通过横向扩散聚集到开放的通道中。这种两步插入-聚集机制的数学描述定量地解释了整个电导-电压动力学,包括失活和其他偏离霍奇金-赫胥利动力学的动力学特征,因为变化的速率常数不仅取决于膜电位,还取决于电导值和时间。所提出的机制也与alamethicin的单通道数据一致,这表明插入和聚集速率常数都是电压相关的。
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