Abad E, Reingruber J, Sansom M S P
Department of Biochemistry, Structural Bioinformatics and Computational Biochemistry Unit, University of Oxford, South Parks Road, Oxford OX1 3QU, United Kingdom.
J Chem Phys. 2009 Feb 28;130(8):085101. doi: 10.1063/1.3077205.
We present a novel rate theory based on the notions of splitting probability and mean first passage time to describe single-ion conduction in narrow, effectively one-dimensional membrane channels. In contrast to traditional approaches such as transition state theory or Kramers theory, transitions between different conduction states in our model are governed by rates which depend on the full geometry of the potential of mean force (PMF) resulting from the superposition of an equilibrium free energy profile and a transmembrane potential induced by a nonequilibrium constraint. If a detailed theoretical PMF is available (e.g., from atomistic molecular dynamics simulations), it can be used to compute characteristic conductance curves in the framework of our model, thereby bridging the gap between the atomistic and the mesoscopic level of description. Explicit analytic solutions for the rates, the ion flux, and the associated electric current can be obtained by approximating the actual PMF by a piecewise linear potential. As illustrative examples, we consider both a theoretical and an experimental application of the model. The theoretical example is based on a hypothetical channel with a fully symmetric sawtooth equilibrium PMF. For this system, we explore how changes in the spatial extent of the binding sites affect the rate of transport when a linear voltage ramp is applied. Already for the case of a single binding site, we find that there is an optimum size of the site which maximizes the current through the channel provided that the applied voltage exceeds a threshold value given by the binding energy of the site. The above optimization effect is shown to arise from the complex interplay between the channel structure and the applied electric field, expressed by a nonlinear dependence of the rates with respect to the linear size of the binding site. In studying the properties of current-voltage curves, we find a double crossover between sublinear and superlinear behaviors as the size of the binding site is varied. The ratio of unidirectional fluxes clearly deviates from the Ussing limit and can be characterized by a flux ratio exponent which decreases below unity as the binding site becomes wider. We also explore effects arising from changes in the ion bulk concentration under symmetric ionic conditions and the presence of additional binding sites in the hypothetical channel. As for the experimental application, we show that our rate theory is able to provide good fits to conductance data for sodium permeation through the gramicidin A channel. Possible extensions of the theory to treat the case of an asymmetric equilibrium PMF, fluctuations in the mean number of translocating ions, the case of fluctuating energy barriers, and multi-ion conductance are briefly discussed.
我们提出了一种基于分裂概率和平均首次通过时间概念的新速率理论,用于描述狭窄的、有效一维膜通道中的单离子传导。与传统方法(如过渡态理论或克莱默斯理论)不同,我们模型中不同传导状态之间的转变由速率控制,这些速率取决于平均力势(PMF)的完整几何形状,该势由平衡自由能分布和非平衡约束引起的跨膜电位叠加而成。如果有详细的理论PMF(例如,来自原子分子动力学模拟),则可以在我们的模型框架内用于计算特征电导曲线,从而弥合原子层面和介观层面描述之间的差距。通过用分段线性势近似实际的PMF,可以得到速率、离子通量和相关电流的显式解析解。作为示例,我们考虑了该模型的理论和实验应用。理论示例基于具有完全对称锯齿形平衡PMF的假设通道。对于这个系统,我们探讨了在施加线性电压斜坡时,结合位点空间范围的变化如何影响传输速率。即使对于单个结合位点的情况,我们发现只要施加的电压超过由位点结合能给出的阈值,就存在一个使通过通道的电流最大化的最佳位点大小。上述优化效应表明是由通道结构和施加电场之间的复杂相互作用引起的,表现为速率相对于结合位点线性大小的非线性依赖关系。在研究电流 - 电压曲线的特性时,我们发现随着结合位点大小的变化,亚线性和超线性行为之间存在双交叉。单向通量的比率明显偏离乌斯廷极限,并且可以用通量比率指数来表征,随着结合位点变宽,该指数降至单位以下。我们还探讨了在对称离子条件下离子体浓度变化以及假设通道中存在额外结合位点所产生的影响。至于实验应用,我们表明我们的速率理论能够很好地拟合通过短杆菌肽A通道的钠渗透的电导数据。简要讨论了该理论可能的扩展,以处理不对称平衡PMF的情况、转运离子平均数的波动、能垒波动的情况以及多离子传导。