TY - JOUR
T1 - Reverse hydrogen spillover onto zeolite-supported metal clusters
T2 - An embedded cluster density functional study of models M6 (M = Rh, Ir, or Au)
AU - Shor, Elena A.Ivanova
AU - Nasluzov, Vladimir A.
AU - Shor, Aleksey M.
AU - Vayssilov, Georgi N.
AU - Rösch, Notker
PY - 2007/8/23
Y1 - 2007/8/23
N2 - A density functional study using isolated cluster models of the zeolite framework (Vayssilov, G. N.; Rösch, N. Phys. Chem. Chem. Phys. 2005, 7, 4019) on supported metal clusters M6/zeo in a hydroxylated faujasite cage showed that for 12 metals M of the groups 8-11 the hydrogenated state, M6(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 M6 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 M6(3H)/zeo: reverse hydrogen spillover from less acidic OH groups onto Au6 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 Au6 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 Rh6 from 123 kJ/mol to 73 and 98 kJ/mol and for Ir6 from 229 kJ/mol to 144 and 160 kJ/mol. We analyzed in detail these differences between the various model approaches.
AB - A density functional study using isolated cluster models of the zeolite framework (Vayssilov, G. N.; Rösch, N. Phys. Chem. Chem. Phys. 2005, 7, 4019) on supported metal clusters M6/zeo in a hydroxylated faujasite cage showed that for 12 metals M of the groups 8-11 the hydrogenated state, M6(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 M6 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 M6(3H)/zeo: reverse hydrogen spillover from less acidic OH groups onto Au6 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 Au6 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 Rh6 from 123 kJ/mol to 73 and 98 kJ/mol and for Ir6 from 229 kJ/mol to 144 and 160 kJ/mol. We analyzed in detail these differences between the various model approaches.
UR - http://www.scopus.com/inward/record.url?scp=34548580795&partnerID=8YFLogxK
U2 - 10.1021/jp0711287
DO - 10.1021/jp0711287
M3 - Article
AN - SCOPUS:34548580795
SN - 1932-7447
VL - 111
SP - 12340
EP - 12351
JO - Journal of Physical Chemistry C
JF - Journal of Physical Chemistry C
IS - 33
ER -