Alternative Low‐Energy Mechanisms for Isotopic Exchange in Gas‐Phase D2O–H+(H2O)n Reactions
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Gaussian 98 (Revision A.7) M. J. Frisch G. W. Trucks H. B. Schlegel G. E. Scuseria M. A. Robb J. R. Cheeseman V. G. Zakrzewski J. A. Montgomery R. E. Stratmann J. C. Burant S. Dapprich J. M. Millam A. D. Daniels K. N. Kudin M. C. Strain O. Farkas J. Tomasi V. Barone M. Cossi R. Cammi B. Mennucci C. Pomelli C. Adamo S. Clifford J. Ochterski G. A. Petersson P. Y. Ayala Q. Cui K. Morokuma D. K. Malick A. D. Rabuck K. Raghavachari J. B. Foresman J. Cioslowski J. V. Ortiz B. B. Stefanov G. Liu A. Liashenko P. Piskorz I. Komaromi R. Gomperts R. L. Martin D. J. Fox T. Keith M. A. Al‐Laham C. Y. Peng A. Nanayakkara C. Gonzalez M. Challacombe P. M. W. Gill B. G. Johnson W. Chen M. W. Wong J. L. Andres M. Head‐Gordon E. S. Replogle J. A. Pople Gaussian Inc. Pittsburgh PA 1998.
The bifurcated processes were found to be roughly 10–20 times less frequent than for instance the water shifts in Figure 3. At the same time the energy barriers for the bifurcated processes were found to be 2–4 kcal mol−1higher than for the water shifts on the OSS2 model surface.
Forst W., 1973, Theory of Unimolecular Reactions
The number of events recorded in the time range of 0–100 ps was found to be substantially larger than at longer times.
The lifetime of the ring isomer was found to be roughly 0.5 ps.
We verified the general correctness of this presupposition allowing water molecules to attach to a cluster with no initial kinetic energy so that it is driven only by the electrostatic interaction with the protonated species. Although one should also expect other docking positions for the incoming D2O especially for larger relative kinetic energy our choice for the initial structure in Scheme 1 represents the worst possible case for the H/D scrambling process as will be apparent in the following.