Gerrard Alex L, Weaver Jason F
Department of Chemical Engineering, University of Florida, Gainesville, FL 32611, USA.
J Chem Phys. 2005 Dec 8;123(22):224703. doi: 10.1063/1.2126667.
Temperature-programmed reaction spectroscopy (TPRS) and direct, isothermal reaction-rate measurements were employed to investigate the oxidation of CO on Pt(111) covered with high concentrations of atomic oxygen. The TPRS results show that oxygen atoms chemisorbed on Pt(111) at coverages just above 0.25 ML (monolayers) are reactive toward coadsorbed CO, producing CO(2) at about 295 K. The uptake of CO on Pt(111) is found to decrease with increasing oxygen coverage beyond 0.25 ML and becomes immeasurable at a surface temperature of 100 K when Pt(111) is partially covered with Pt oxide domains at oxygen coverages above 1.5 ML. The rate of CO oxidation measured as a function of CO beam exposure to the surface exhibits a nearly linear increase toward a maximum for initial oxygen coverages between 0.25 and 0.50 ML and constant surface temperatures between 300 and 500 K. At a fixed CO incident flux, the time required to reach the maximum reaction rate increases as the initial oxygen coverage is increased to 0.50 ML. A time lag prior to the reaction-rate maximum is also observed when Pt oxide domains are present on the surface, but the reaction rate increases more slowly with CO exposure and much longer time lags are observed, indicating that the oxide phase is less reactive toward CO than are chemisorbed oxygen atoms on Pt(111). On the partially oxidized surface, the CO exposure needed to reach the rate maximum increases significantly with increases in both the initial oxygen coverage and the surface temperature. A kinetic model is developed that reproduces the qualitative dependence of the CO oxidation rate on the atomic oxygen coverage and the surface temperature. The model assumes that CO chemisorption and reaction occur only on regions of the surface covered by chemisorbed oxygen atoms and describes the CO chemisorption probability as a decreasing function of the atomic oxygen coverage in the chemisorbed phase. The model also takes into account the migration of oxygen atoms from oxide domains to domains with chemisorbed oxygen atoms. According to the model, the reaction rate initially increases with the CO exposure because the rate of CO chemisorption is enhanced as the coverage of chemisorbed oxygen atoms decreases during reaction. Longer rate delays are predicted for the partially oxidized surface because oxygen migration from the oxide phase maintains high oxygen coverages in the coexisting chemisorbed oxygen phase that hinder CO chemisorption. It is shown that the time evolution of the CO oxidation rate is determined by the relative rates of CO chemisorption and oxygen migration, R(ad) and R(m), respectively, with an increase in the relative rate of oxygen migration acting to inhibit the reaction. We find that the time lag in the reaction rate increases nearly exponentially with the initial oxygen coverage O (tot) when O (tot) exceeds a critical value, which is defined as the coverage above which R(ad)R(m) is less than unity at fixed CO incident flux and surface temperature. These results demonstrate that the kinetics for CO oxidation on oxidized Pt(111) is governed by the sensitivity of CO binding and chemisorption on the atomic oxygen coverage and the distribution of surface oxygen phases.
采用程序升温反应光谱法(TPRS)以及直接等温反应速率测量法,研究了在覆盖高浓度原子氧的Pt(111)上CO的氧化反应。TPRS结果表明,覆盖度略高于0.25 ML(单层)时化学吸附在Pt(111)上的氧原子对共吸附的CO具有反应活性,在约295 K时生成CO₂。当氧覆盖度超过0.25 ML时,发现CO在Pt(111)上的吸附量随氧覆盖度的增加而减少,当氧覆盖度高于1.5 ML时,Pt(111)部分被Pt氧化物畴覆盖,在100 K的表面温度下,CO的吸附量变得无法测量。以CO束流对表面的曝光量为函数测量的CO氧化速率,对于初始氧覆盖度在0.25至0.50 ML之间且表面温度在300至500 K之间的情况,呈现出接近线性增加直至最大值,然后保持恒定。在固定的CO入射通量下,随着初始氧覆盖度增加到0.50 ML,达到最大反应速率所需的时间增加。当表面存在Pt氧化物畴时,在反应速率达到最大值之前也观察到了时间滞后,但反应速率随CO曝光的增加更为缓慢,并且观察到更长的时间滞后,这表明氧化物相对CO的反应活性低于Pt(111)上化学吸附的氧原子。在部分氧化的表面上,达到速率最大值所需的CO曝光量随着初始氧覆盖度和表面温度的增加而显著增加。建立了一个动力学模型,该模型再现了CO氧化速率对原子氧覆盖度和表面温度的定性依赖关系。该模型假设CO的化学吸附和反应仅发生在被化学吸附氧原子覆盖的表面区域,并将CO化学吸附概率描述为化学吸附相中原子氧覆盖度的递减函数。该模型还考虑了氧原子从氧化物畴向具有化学吸附氧原子的畴的迁移。根据该模型,反应速率最初随CO曝光而增加,因为在反应过程中随着化学吸附氧原子覆盖度的降低,CO化学吸附速率增强。对于部分氧化的表面,预测会有更长的速率延迟,因为从氧化物相迁移的氧在共存的化学吸附氧相中维持了高氧覆盖度,从而阻碍了CO的化学吸附。结果表明,CO氧化速率的时间演化分别由CO化学吸附速率和氧迁移速率R(ad)和R(m)决定,氧迁移相对速率的增加起到抑制反应的作用。我们发现,当O(tot)超过一个临界值时,反应速率的时间滞后几乎随初始氧覆盖度O(tot)呈指数增加,该临界值定义为在固定的CO入射通量和表面温度下,R(ad)R(m)小于1的覆盖度。这些结果表明,氧化的Pt(111)上CO氧化的动力学受CO结合和化学吸附对原子氧覆盖度以及表面氧相分布的敏感性控制。