French R J
Biophys J. 1977 Apr;18(1):53-61. doi: 10.1016/S0006-3495(77)85596-3.
The potential difference between two solutions of the same 1:1 electrolyte bathing an ion exchange membrane has been calculated as the sum of the following components: (a) a Donnan potential at each membrane-solution interface, (b) a diffusion potential within the membrane phase, and (c) a diffusion potential in the unstirred layer on each side of the membrane. For a highly charged ion exchange membrane with at least one surface in contact with a dilute solution, calculated transmembrane potential differences are extremely sensitive to the assumed thickness of the unstirred layers. This sensitivity to unstirred layer thickness is primarily due to changes in the Donnan components of the potential difference. By this approach, it was possible to fit membrane potential data from Gunn and Curran (1971, Biophys. J. 11:559) for a range of bathing solution concentrations from 0.0016 to 4.0 M. If no effort was made to account for the modification of the Donnan potentials by the presence of unstirred layers, the data appeared incompatible with an electrodiffusion equation description. Suggestions for a more stringent experimental test and a brief discussion of possible implications for electrical measurements on fresh-water giant algal cells are presented.
同一1:1电解质的两种溶液浸泡离子交换膜时,其电位差可计算为以下各部分之和:(a) 每个膜-溶液界面处的唐南电位;(b) 膜相内的扩散电位;(c) 膜两侧未搅拌层中的扩散电位。对于至少有一个表面与稀溶液接触的高电荷离子交换膜,计算得到的跨膜电位差对未搅拌层的假定厚度极为敏感。这种对未搅拌层厚度的敏感性主要是由于电位差的唐南分量发生了变化。通过这种方法,可以拟合Gunn和Curran(1971年,《生物物理杂志》11:559)在0.0016至4.0 M一系列浸泡溶液浓度下的膜电位数据。如果不考虑未搅拌层的存在对唐南电位的修正,数据似乎与电扩散方程描述不相符。本文提出了更严格实验测试的建议,并简要讨论了对淡水巨型藻类细胞电测量可能产生的影响。