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Royal Society of Chemistry, Dalton Transactions, 19(44), p. 9200-9208, 2015

DOI: 10.1039/c5dt00978b

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Mechanistic insights into the full hydrogenation of 2,6-substituted pyridine catalyzed by the Lewis acid C<sub>6</sub>F<sub>5</sub>(CH<sub>2</sub>)<sub>2</sub>B(C<sub>6</sub>F<sub>5</sub>)<sub>2</sub>

Journal article published in 2015 by Jiyang Zhao, Guoqiang Wang, Shuhua Li ORCID
This paper was not found in any repository, but could be made available legally by the author.
This paper was not found in any repository, but could be made available legally by the author.

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Abstract

The reaction mechanism for the full hydrogenation of 2-phenyl-6-methyl-pyridine catalyzed by the Lewis acid C6F5(CH2)2B(C6F5)2 was investigated in detail by density functional theory calculations. Our calculations show that a plausible reaction pathway of the hydrogenation of pyridine contains five stages: (1) the generation of a new borane C6F5(CH2)2B(C6F5)2 from the hydroboration of the alkene, which forms a frustrated Lewis pair (FLP) with a pyridine; (2) the activation of H2 by FLP to yield an ion pair intermediate; (3) intramolecular hydride transfer from the boron atom to the pyridinium cation in the ion pair intermediate to produce the 1,4-dihydropyridine; (4) hydrogenation of the 1,4-dihydropyridine by the FLP to form the 1,4,5,6-tetrahydropyridine; (5) hydrogenation of the 1,4,5,6-tetrahydropyridine by the FLP to yield the final piperidine. The last two hydrogenation processes follow a similar pathway, which includes four steps: (a) proton transfer from the pyridinium moiety to the substrate; (b) dissociation of the newly generated pyridine; (c) hydride migration from the hydridoborate moiety to the protonated substrate to produce the hydrogenated product; (d) release of the hydrogenated product to regenerate the free borane. The full hydrogenation of pyridine is calculated to be exothermic by 16.9 kcal mol(-1), relative to the starting reactants. The rate-limiting step is the proton transfer in the second hydrogenation step, with a free energy barrier of 28.2 kcal mol(-1) in the gas phase (27.9 kcal mol(-1) in toluene) at room temperature and 1.0 atm. Our results can account for the observed experimental facts.