Nonner W, Chen D P, Eisenberg B
Department of Physiology and Biophysics, University of Miami School of Medicine, Florida 33101-4819, USA.
Biophys J. 1998 May;74(5):2327-34. doi: 10.1016/S0006-3495(98)77942-1.
Ionic channels bathed in mixed solutions of two permeant electrolytes often conduct less current than channels bathed in pure solutions of either. For many years, this anomalous mole fraction effect (AMFE) has been thought to occur only in single-file pores containing two or more ions at a time. Most thinking about channels incorporates this view. We show here that the AMFE arises naturally, as an electrostatic consequence of localized ion specific binding, if the average current through a channel is described by a theory (Poisson-Nernst-Planck, PNP) that computes the average electric field from the average concentration of charges in and near the channel. The theory contains only those ion-ion interactions mediated by the mean field, and it does not enforce single filing. The AMFE is predicted by PNP over a wide range of mean concentrations of ions in the channel; for example, it is predicted when (on the average) less, or much less, than one ion is found in the channel's pore. In this treatment, the AMFE arises, in large measure, from a depletion layer produced near a region of ion-specific binding. The small excess concentration of ions in the binding region repels all nearby ions of like charge, thereby creating a depletion layer. The overall conductance of the channel arises in effect from resistors in series, one from the binding region, one from the depletion zone, and one from the unbinding region. The highest value resistor (which occurs in the depletion zone) limits the overall series conductance. Here the AMFE is not the result of single filing or multiple occupancy, and so previous views of permeation need to be revised: the presence of an AMFE does not imply that ions permeate single file through a multiply occupied pore.
浸泡在两种可渗透电解质混合溶液中的离子通道,其传导的电流通常比浸泡在任何一种纯溶液中的通道传导的电流要少。多年来,人们一直认为这种异常摩尔分数效应(AMFE)仅发生在每次含有两个或更多离子的单排孔中。大多数关于通道的观点都包含了这一观点。我们在此表明,如果通过通道的平均电流由一种理论(泊松 - 能斯特 - 普朗克,PNP)来描述,该理论根据通道内及附近电荷的平均浓度计算平均电场,那么AMFE会作为局部离子特异性结合的静电结果自然出现。该理论仅包含由平均场介导的离子 - 离子相互作用,并且不强制单排排列。PNP在通道中离子的广泛平均浓度范围内都预测到了AMFE;例如,当(平均而言)在通道孔中发现的离子少于一个或远少于一个时,就会预测到AMFE。在这种处理中,AMFE在很大程度上源于离子特异性结合区域附近产生的耗尽层。结合区域中离子的少量过量浓度排斥所有附近相同电荷的离子,从而形成一个耗尽层。通道的整体电导率实际上源于串联的电阻器,一个来自结合区域,一个来自耗尽区,一个来自非结合区域。阻值最高的电阻器(出现在耗尽区)限制了整体串联电导率。在此,AMFE不是单排排列或多重占据的结果,因此先前的渗透观点需要修正:AMFE的存在并不意味着离子通过多重占据的孔单排渗透。