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首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >Roles of Proton and Electric Field in the Electroreduction of O_2 on Pt(111) Surfaces: Results of an Ab-Initio Molecular Dynamics Study
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Roles of Proton and Electric Field in the Electroreduction of O_2 on Pt(111) Surfaces: Results of an Ab-Initio Molecular Dynamics Study

机译:质子和电场在Pt(111)表面O_2电还原中的作用:从头算分子动力学研究的结果

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The electroreduction of O_2 on the Pt(111) surface is studied with Car-Parrinello molecular dynamics simulations of O_2/Pt(111), O_2 + H~+(H_2O)_3/Pt(111), and O_2 + H~+(H_2O)_3 + e~-/ Pt(111). Starting from a parallel configuration where O_2 is 3.0 A over the Pt(111) surface along a bridge site, stepwise adsorptions of two oxygen atoms are observed, leading to a one-end chemisorption precursor (Pauling model of adsorption). The formation of the precursor has a very low barrier (0.08 eV), whereas no clear barrier was found for its decomposition. Addition of H~+(H_2O)_3 induces rapid formation of the proton-transfer intermediate H~+-O_2···Pt(111), followed by an electron transfer from the Pt slab that yields a chemisorbed precursor H-O-O-Ptn, in which the hydroxyl end is considerably more separated than the oxygen end from the Pt(111) surface. Compared with the O_2 + H~+(H_2O)_3/Pt(111) system, the presence of an electron in O_2 + H~+(H_2O)_3 + e~-/ Pt(111) greatly enhances the lifetime of the proton-transfer intermediate H~+-O-O···Pt(111), and consequently it delays the subsequent electron transfer, which yields the formation of the one-end chemisorbed precursor H-O-O-Pt_n. Evolutions of the Kohn-Sham energy for the last two cases show that the formation of H-O-O-Pt_n has a much higher activation barrier than its dissociation (0.4 vs 0.1 eV), indicating that the formation of chemisorbed H-O_2 species is the rate-determining step for the first electron transfer of the electroreduction of O_2.
机译:通过O_2 / Pt(111),O_2 + H〜+(H_2O)_3 / Pt(111)和O_2 + H〜+()的Car-Parrinello分子动力学模拟研究了Pt(111)表面上O_2的电还原H_2O)_3 + e〜-/ Pt(111)。从O_2在Pt(111)面上沿着桥位点的O_2为3.0 A的平行构型开始,观察到两个氧原子的逐步吸附,导致了一个单端化学吸附前体(鲍林吸附模型)。前体的形成具有非常低的势垒(0.08 eV),而未发现明确的势垒可用于分解。 H〜+(H_2O)_3的添加会引起质子转移中间体H〜+ -O_2··Pt(111)的快速形成,随后电子从Pt平板转移,产生化学吸附的前体HOO-Ptn。 Pt(111)表面的羟基末端比氧末端明显更多。与O_2 + H〜+(H_2O)_3 / Pt(111)体系相比,O_2 + H〜+(H_2O)_3 + e〜-/ Pt(111)中电子的存在大大提高了质子的寿命-转移中间体H〜+ -OO··Pt(111),因此它延迟了随后的电子转移,从而形成了一端化学吸附的前体HOO-Pt_n。最近两种情况下Kohn-Sham能量的演变表明,HOO-Pt_n的形成比其解离具有更高的活化势垒(0.4 vs 0.1 eV),这表明化学吸附的H-O_2物种的形成是确定O 2的电还原的第一次电子转移的步骤。

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