Tanaka Kazuyuki, Nishi Naoya, Kakiuchi Takashi
Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Nishikyoku, Kyoto 615-8510, Japan.
Anal Sci. 2004 Nov;20(11):1553-7. doi: 10.2116/analsci.20.1553.
The electrode reaction of decamethylferrocene (DMFc) dissolved in a thin layer of a room-temperature molten salt (RTMS), 1-octyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide (C8mimC1C1N) or 1-octyl-3-methylimidazolium bis(pentafluoroethylsulfonyl)imide (C8mimC2C2N), on a self-assembled monolayer-modified gold electrode is coupled with the ion transfer across the interface between the RTMS and the outer aqueous solution (W) to give a voltammogram whose shape resembles a voltammogram of a simple one-electron transfer process. The electroneutrality of the RTMS layer during the oxidation of DMFc to decamethylferricenium ion is maintained by the concomitant dissolution of C8mim+ ion from the RTMS phase to the W phase, and the reduction of decamethylferricenium ion to DMFc is accompanied by the transfer of either C1C1N- or C2C2N- from RTMS to W. The midpoint potential of the voltammogram varies with the concentration of the salt in the aqueous phase, C8mimCl or LiCnCnN (n = 1 or 2), in a Nernstian manner, showing that the phase-boundary potential between the RTMS and the W is controlled by the partition of these ions. Although the phase-boundary potential across the RTMS / W interface is Nernstian with respect to the ions common to both phases at the equilibrium, the polarization at the RTMS / W interface under current flow distorts the shape of the voltammograms, resulting in a wider peak separation in the voltammogram.
溶解在室温熔盐(RTMS)薄层中的十甲基二茂铁(DMFc),即1-辛基-3-甲基咪唑双(三氟甲基磺酰)亚胺(C8mimC1C1N)或1-辛基-3-甲基咪唑双(五氟乙基磺酰)亚胺(C8mimC2C2N),在自组装单层修饰金电极上的电极反应与离子在RTMS和外部水溶液(W)之间的界面上的转移相耦合,从而得到一个伏安图,其形状类似于简单单电子转移过程的伏安图。在DMFc氧化为十甲基二茂铁离子的过程中,RTMS层的电中性通过C8mim +离子从RTMS相伴随溶解到W相来维持,而十甲基二茂铁离子还原为DMFc则伴随着C1C1N-或C2C2N-从RTMS转移到W。伏安图的中点电位以能斯特方式随水相中盐的浓度,即C8mimCl或LiCnCnN(n = 1或2)而变化,表明RTMS和W之间的相界电位由这些离子的分配控制。尽管在平衡时,跨RTMS / W界面的相界电位相对于两相共有的离子是能斯特的,但电流流动时RTMS / W界面处的极化会使伏安图的形状失真,导致伏安图中的峰间距变宽。