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Applicability and limits of the ensemble model in catalysis by metals: The kinetics of ethane hydrogenolysis over Pt/SiO2

机译:整体模型在金属催化中的适用性和局限性:Pt / SiO2上乙烷加氢反应动力学

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The rate of ethane hydrogenolysis over the EUROPT 1 (Pt/SiO2) catalyst has been studied over a large range of pressure and temperature. At ethane pressures, P-E, lower than 1.3 kPa the hydrocarbon coverage is shown to be negligible. For T, P conditions which correspond to a degree of hydrogen coverage, theta(H), below 0.6 ML (monolayer), the rate r is found to be related to theta(H) and P-E, by the equation, r = k(0)P(E)e(-E0/RT)(1 - beta theta(H))(X), With k(0) approximately 4 times smaller than the number of ethane molecules colliding with the Pt surface, E-0 = 55 +/- 7 kJ mol(-1), X = 9 +/- 2, and beta = 1.3 +/- 0.1. This rate equation which models on a quantitative ground the complex variations of r with T and P might be considered as describing a two-body process between gaseous ethane and surface ensembles composed of X adjacent platinum atoms free from adsorbed hydrogen, Eo being the activation energy. The constant beta takes into consideration the fact that at saturation the surface stoichiometry H/Pt-s is larger than unity. In a T, P domain which corresponds to hydrogen coverage above 0.6 ML, a marked change in the evolution of the kinetic parameters is observed: the apparent activation energy starts to decrease and the order versus the hydrogen pressure starts to be less negative by decreasing the temperature. The above purely statistical model does not apply anymore to this kinetic domain, which could be characterised by some H adsorption ordering. This work shows that the ensemble model, successfully applied to describe catalytic reactions occurring over Rh and Ni catalysts, can be extended to the case of Pt, within a domain characterized by a moderate hydrogen coverage and a purely statistical adsorption process. (C) 1998 Academic Press. [References: 33]
机译:在较大的压力和温度范围内,已经研究了在EUROPT 1(Pt / SiO2)催化剂上乙烷的氢解速率。在乙烷压力P-E低于1.3 kPa时,碳氢化合物的覆盖率可以忽略不计。对于与氢覆盖度theta(H)相对应的T,P条件(低于0.6 ML(单层)),速率r与theta(H)和PE有关,通过等式r = k( 0)P(E)e(-E0 / RT)(1-βtheta(H))(X),其中k(0)小于与Pt表面碰撞的乙烷分子数量的4倍,E-0 = 55 +/- 7 kJ mol(-1),X = 9 +/- 2,β= 1.3 +/- 0.1。该速率方程在定量基础上模拟了r随T和P的复杂变化,可以认为是描述了气态乙烷与由X个相邻的无吸附氢的铂原子组成的表面团簇之间的两体过程,Eo是活化能。常数β考虑到以下事实:饱和时,表面化学计量比H / Pt-s大于1。在对应于高于0.6 ML的氢覆盖范围的T,P域中,观察到动力学参数演变的显着变化:表观活化能开始降低,并且随着氢压降的降低,相对于氢压的阶次开始减小。温度。上述纯粹的统计模型不再适用于该动力学域,该动力学域可以通过某些H吸附排序来表征。这项工作表明,成功地用于描述在Rh和Ni催化剂上发生的催化反应的集成模型可以扩展到Pt的情况下,其特征是具有适度的氢覆盖范围和纯粹的统计吸附过程。 (C)1998年学术出版社。 [参考:33]

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