Passage of Diffusion-Migration Current Across Electrode/Membrane/Solution System. Part 1: Short-Time Evolution. Binary Electrolyte (Equal Mobilities)

IF 1.1 4区 工程技术 Q4 ELECTROCHEMISTRY
M. A. Vorotyntsev, P. A. Zader
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引用次数: 0

Abstract

The express-method proposed recently for experimental determination of diffusion coefficients of electroactive ions inside a membrane and their distribution coefficients at the membrane/solution boundary (Russ. J. Electrochem., 2022, 58, 1103) is based on the comparison of the measured non-stationary current for the electrode/membrane/electrolyte solution system upon the applying of a potential step with the theoretical expressions for the current–time dependence. Application of this method for the study of bromide-anion transport across the membrane was performed in the previous work under the condition of the membrane permselectivity where the amplitude of the electric field inside the membrane was suppressed owing to a high concentration of non-electroactive counterions. Then, the coion (bromide anion) transport occurred by the diffusional mechanism, for which the solution was available in an analytical form. The present study considers for the first time a non-stationary electrodiffusional transmembrane transport of two singly charged ions (e.g., background cation М+ as the counterion and electroactive anion X as the coion) having identical diffusion coefficients where the current passage induced a transient electric field in this space, resulting in a deviation from predictions for the diffusional mechanism. It is found that within the short time interval after the applying of the potential step from the membrane equilibrium state to the limiting current regime (where the thickness of the non-stationary diffusion layer is significantly smaller than that of the membrane) the non-stationary distributions of the ion concentrations and of the electric field strength as a function of two variables (the spatial and temporal ones, x and t) can be expressed via a function of one variable, Z(z), where z = x/(4Dt)1/2. The form of the expression, depending on the ratio of the surface concentration of component X to the fixed charge density inside the membrane (Xm/Cf) has been found by numerical integration. The limiting current varies with time according to the Cottrell formula (I ~ t–1/2); the dependence of the dimensionless current amplitude, i, on the Xm/Cf ratio is found by numerical calculation; an approximate analytical formula has also been proposed. In particular, the passing current is shown to be close to the diffusion-limited one for a low coion concentration at the membrane/electrolyte solution boundary as compared with the concentration of immobile charged groups inside the membrane (Xm/Cf \( \ll \) 1), whereas the migration contribution to the ionic fluxes doubles the limiting current when the opposite condition (Xm/Cf \( \gg \) 1) is fulfilled.

Abstract Image

Abstract Image

穿越电极/膜/溶液系统的扩散-迁移电流。第 1 部分:短时间演变。二元电解质(等迁移率)
摘要 最近提出的实验测定膜内电活性离子扩散系数及其在膜/溶液边界分布系数的快速方法(Russ. J. Electrochem.在之前的工作中,在膜过选择性条件下应用这种方法研究了溴阴离子在膜上的传输,由于高浓度的非电活性反离子,膜内电场的振幅被抑制。然后,辅离子(溴阴离子)通过扩散机制进行传输,而这一机制的解决方案是以分析形式提供的。本研究首次考虑了具有相同扩散系数的两个单电荷离子(如作为反离子的本底阳离子М+和作为辅离子的电活性阴离子X-)的非稳态电扩散跨膜传输,在这种情况下,电流通过会在该空间诱发瞬态电场,从而导致与扩散机制的预测出现偏差。研究发现,在施加从膜平衡态到极限电流状态的电位阶跃后的短时间间隔内(此时非稳态扩散层的厚度明显小于膜的厚度),离子浓度和电场强度的非稳态分布作为两个变量(空间变量和时间变量 x 和 t)的函数,可以通过一个变量 Z(z) 的函数来表示,其中 z = x/(4Dt)1/2。表达式的形式取决于成分 X 的表面浓度与膜内固定电荷密度的比率(Xm/Cf)。极限电流根据科特雷尔公式(I ~ t-1/2)随时间变化;无量纲电流振幅 i 与 Xm/Cf 比率的关系通过数值计算得出;同时还提出了一个近似解析公式。特别是,与膜内不动带电基团的浓度(Xm/Cf \( \ll \) 1)相比,当膜/电解质溶液边界的共离子浓度较低时,通过电流接近于扩散极限电流,而当满足相反条件(Xm/Cf \( \gg \) 1)时,离子通量的迁移贡献使极限电流翻倍。
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来源期刊
Russian Journal of Electrochemistry
Russian Journal of Electrochemistry 工程技术-电化学
CiteScore
1.90
自引率
8.30%
发文量
102
审稿时长
6 months
期刊介绍: Russian Journal of Electrochemistry is a journal that covers all aspects of research in modern electrochemistry. The journal welcomes submissions in English or Russian regardless of country and nationality of authors.
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