Department of Physical Sciences (CHEMISTRY), The University of Hull, Kingston-upon-Hull, United Kingdom.
J Phys Chem B. 2011 May 26;115(20):6509-23. doi: 10.1021/jp201806f. Epub 2011 May 2.
The H(1) lyotropic liquid crystalline phase of Triton X 100 with aqueous 0.1 M potassium chloride is examined as a medium in which to determine the axiosymmetric anisotropy in the diffusion flux of N,N,N',N'-tetramethyl-para-phenylenediamine using electrochemical methods (voltammetry and potential step chronoamperometry) at both planar electrodes and two-dimensional flux microdisk electrodes. Comparison of experiment with theory suggests the ratio of anisotropic diffusion coefficients in the directions tangential and perpendicular to the electrode surface varies over two orders of magnitude (from 0.04 to 3.3) with increasing concentration of the redox analyte. This is understood through the occurrence of a long-range charge transfer across the pseudophase | pseudophase boundary interface, occurring as a result of differential diffusivities of the redox probe within the surfactant and aqueous subphases. These data and their dependence on the analyte concentration empower, in a proof-of-concept, the estimation of the partition equilibrium constant (K(P)); the value estimated for the small electroactive-drug mimetic considered is log K(P) = 2.01 ± 0.05 (at 294 ± 2 K) and is in agreement with that envisaged for its partition between n-octanol and water. It is suggested that only measurements at low analyte loadings allow for interphase electron transfers to be neglected, since then percolation effects appear to dominate the Faradaic current.
用电化学方法(伏安法和电位阶跃计时安培法)在平面电极和二维通量微盘电极上研究了 Triton X-100 与 0.1 M 氯化钾水溶液的 H(1)溶致液晶相作为介质,以确定 N,N,N',N'-四甲基对苯二胺在扩散通量中的轴对称各向异性。实验与理论的比较表明,随着氧化还原分析物浓度的增加,沿电极表面切向和垂直方向的各向异性扩散系数之比变化了两个数量级(从 0.04 到 3.3)。这是由于在赝相与赝相边界界面上发生长程电荷转移,这是由于氧化还原探针在表面活性剂和水亚相中不同的扩散系数所致。这些数据及其对分析物浓度的依赖性,在概念验证中,能够估计分配平衡常数(K(P));对于所考虑的小电活性药物模拟物,估计的值为 log K(P)= 2.01 ± 0.05(在 294 ± 2 K 下),与它们在正辛醇和水之间的分配一致。有人认为,只有在低分析物负荷下的测量才能忽略相间电子转移,因为那时渗流效应似乎主导了法拉第电流。