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质子转移到带电的铂电极。分子动力学轨迹研究。

Proton transfer to charged platinum electrodes. A molecular dynamics trajectory study.

机构信息

Institute of Theoretical Chemistry, Ulm University, D-89069 Ulm, Germany.

出版信息

J Phys Condens Matter. 2010 May 5;22(17):175001. doi: 10.1088/0953-8984/22/17/175001. Epub 2010 Mar 23.

Abstract

A recently developed empirical valence bond (EVB) model for proton transfer on Pt(111) electrodes (Wilhelm et al 2008 J. Phys. Chem. C 112 10814) has been applied in molecular dynamics (MD) simulations of a water film in contact with a charged Pt surface. A total of seven negative surface charge densities σ between -7.5 and -18.9 µC cm(-2) were investigated. For each value of σ, between 30 and 84 initial conditions of a solvated proton within a water slab were sampled, and the trajectories were integrated until discharge of a proton occurred on the charged surfaces. We have calculated the mean rates for discharge and for adsorption of solvated protons within the adsorbed water layer in contact with the metal electrode as a function of surface charge density. For the less negative values of σ we observe a Tafel-like exponential increase of discharge rate with decreasing σ. At the more negative values this exponential increase levels off and the discharge process is apparently transport limited. Mechanistically, the Tafel regime corresponds to a stepwise proton transfer: first, a proton is transferred from the bulk into the contact water layer, which is followed by transfer of a proton to the charged surface and concomitant discharge. At the more negative surface charge densities the proton transfer into the contact water layer and the transfer of another proton to the surface and its discharge occur almost simultaneously.

摘要

最近开发的用于 Pt(111)电极质子转移的经验价电子键 (EVB) 模型(Wilhelm 等人,2008 年,J. Phys. Chem. C 112, 10814)已应用于与带电 Pt 表面接触的水膜的分子动力学 (MD) 模拟。总共研究了七种负表面电荷密度 σ,范围在-7.5 到-18.9 µC cm(-2) 之间。对于每个 σ 值,在一个水分子层内有一个溶剂化质子的 30 到 84 个初始条件被采样,并且轨迹被积分,直到质子在带电表面上放电。我们已经计算了在与金属电极接触的吸附水层内溶剂化质子的放电和吸附的平均速率作为表面电荷密度的函数。对于较小的 σ 值,我们观察到放电速率随着 σ 的减小呈 Tafel 样指数增加。在更负的 σ 值下,这种指数增加趋于平稳,放电过程显然受到传输限制。从机理上讲,Tafel 区对应于逐步质子转移:首先,质子从本体转移到接触水层,然后质子转移到带电表面并伴随放电。在更负的表面电荷密度下,质子转移到接触水层和另一个质子转移到表面及其放电几乎同时发生。

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