account for the greater deviation of the S–C–F angle in TS2
(156.51) from the ideal value of 1801 than in TS1 (171.91).
The calculated values for the reaction barriers assess the role
of the OH group adjacent to the C–F bond in assisting the
release of the fluoride leaving group. The gas-phase energy
barrier calculated for the reaction between 1 and 2 is 44.7 kcal
molꢁ1, and that for 2 and 4 is 51.9 kcal molꢁ1. When the
solvent toluene is included in the calculation by the PCM
method, the difference in the energy barriers for these two
reactions is even larger, with values of 36.6 and 46.4 kcal
molꢁ1, respectively. These theoretical results agree well with
the experimental observation that 2 does react with 1 but it
does not with 4. In addition, the large value of the activation
energy barrier agrees well with the experimental conditions
required for the reaction of 1 with 2 (refluxing toluene).
Overall, we have shown that the presence of the OH group
stabilizes the transition state by means of the Fꢀ ꢀ ꢀH–O supra-
molecular interaction that provides an electrophilic assistance
to the C–F cleavage.
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Hydrogen bond interactions have been proved in this work
as an efficient way to assist the C–F activation. The assistance
here reported has been provided by an OH group enclosed in
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The authors thank the financial support from the Ministerio
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18. The geometries of the minima and transition states were fully
optimized at the B3LYP level and the energies here presented were
those obtained from single point calculations at the MP2 level. See
supporting informationw for more detail.
de Ciencia y Tecnologı
and CTQ2005-09000-C02-01). G. U. and R. M. B. thank the
Spanish MEC for funding through the ‘‘Ramon y Cajal’’
´
a of Spain (projects CTQ2004-01463
´
program.
Notes and references
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ꢂc
This journal is The Royal Society of Chemistry 2008
3132 | Chem. Commun., 2008, 3130–3132