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首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Reverse hydrogen spillover onto zeolite-supported metal clusters: An embedded cluster density functional study of models M-6 (M = Rh, Ir, or Au)
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Reverse hydrogen spillover onto zeolite-supported metal clusters: An embedded cluster density functional study of models M-6 (M = Rh, Ir, or Au)

机译:反向氢气溢出到沸石负载的金属团簇上:模型M-6(M = Rh,Ir或Au)的嵌入团簇密度泛函研究

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摘要

A density functional study using isolated cluster models of the zeolite framework (Vayssilov, G. N.; Rosch, N. Phys. Chem. Chem. Phys. 2005, 7, 4019) on supported metal clusters M-6/zeo in a hydroxylated faujasite cage showed that for 12 metals M of the groups 8-11 the hydrogenated state, M-6(3H)/zeo, is energetically preferred over the bare form M-6/zeo(3H). The former state was obtained as result of reverse hydrogen spillover from zeolite OH groups onto the metal particle. In the present work, we reinvestigated this problem of identifying the favorable chemical state of zeolite-supported metal species for selected M-6 model clusters (M = Rh, Ir, or Au) using an accurate quantum mechanics/molecular mechanics (QM/MM) approach where a QM partition is embedded in an extended zeolite lattice (MM). The embedding method covEPE, an improved variant of the elastic polarizable environment model EPE, adapted for polar-covalent materials, properly accounts for both the mechanical rigidity of the zeolite framework and the electrostatic field due to the infinite lattice. With this method, we discovered the first example where the bare zeolite-supported form M-6/zeo(3H) is energetically preferred over the hydrogenated from M-6(3H)/zeo: reverse hydrogen spillover from less acidic OH groups onto Au-6 was calculated to be endothermic, on average by 29 kJ/mol per transferred proton. In contrast, reverse spillover from the more acidic hydroxyl groups to Au-6 is exothermic by 47 kJ/mol per proton. For the other metals, the QM/MM approach predicts reverse hydrogen spillover to be energetically favorable, just as the simple model approach with finite models of the zeolite support. However, the corresponding calculated energy change is strongly reduced (per proton) for Rh-6 from 123 kJ/mol to 73 and 98 kJ/mol and for Ir-6 from 229 kJ/mol to 144 and 160 kJ/mol. We analyzed in detail these differences between the various model approaches.
机译:使用分子筛骨架的孤立簇模型(Vayssilov,GN; Rosch,N.Phys.Chem.Chem.Phys.2005,7,4019)在羟基八面沸石笼中的支撑金属簇M-6 / zeo上进行密度泛函研究对于第8-11族的12种金属M而言,相对于裸露的M-6 / zeo(3H),在能量上优选氢化态M-6(3H)/ zeo。前一种状态是由于氢从沸石OH基团反向溢出到金属颗粒上而获得的。在当前的工作中,我们重新研究了使用精确的量子力学/分子力学(QM / MM)为选定的M-6模型簇(M = Rh,Ir或Au)确定沸石负载的金属物种的有利化学状态的问题。 )方法,将QM分区嵌入扩展的沸石晶格(MM)中。嵌入方法covEPE是弹性可极化环境模型EPE的改进变体,适用于极性共价材料,可适当考虑沸石骨架的机械刚度和无限晶格引起的静电场。通过这种方法,我们发现了第一个例子,即从能量上优先于M-6(3H)/ zeo的氢化反应,优先选择裸沸石负载的M-6 / zeo(3H)形式:将氢从酸性较低的OH基团逆向溢出到Au上-6被计算为吸热的,平均每个转移的质子为29 kJ / mol。相反,从更酸性的羟基到Au-6的反向溢出是每质子47 kJ / mol放热。对于其他金属,QM / MM方法预测反向氢气溢出在能量上是有利的,就像使用沸石载体有限模型的简单模型方法一样。但是,Rh-6的相应计算的能量变化(每个质子)从123 kJ / mol大大降低到73和98 kJ / mol,Ir-6从229 kJ / mol降低到144和160 kJ / mol。我们详细分析了各种模型方法之间的这些差异。

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