posted on 2015-03-26, 00:00authored byIstván Szabó, Gábor Czakó
The
double-inversion and front-side attack transition states as well as
the proton-abstraction channels of the X– + CH3Y [X,Y = F, Cl, Br, I] reactions are characterized by the
explicitly correlated CCSD(T)-F12b/aug-cc-pVTZ(-PP) level of theory
using small-core relativistic effective core potentials and the corresponding
aug-cc-pVTZ-PP bases for Br and I. In the X = F case the double-inversion
classical(adiabatic) barrier heights are 28.7(25.6), 15.8(13.4), 13.2(11.0),
and 8.6(6.6) kcal mol–1 for Y = F, Cl, Br, and I,
respectively, whereas the barrier heights are in the 40–90
kcal mol–1 range for the other 12 reactions. The
abstraction channels are always above the double-inversion saddle
points. For X = F, the front-side attack classical(adiabatic) barrier
heights, 45.8(44.8), 31.0(30.3), 24.7(24.2), and 19.5(19.3) kcal mol–1 for Y = F, Cl, Br, and I, respectively, are higher
than the corresponding double-inversion ones, whereas for the other
systems the front-side attack saddle points are in the 35–70
kcal mol–1 range. The double-inversion transition
states have XH···CH2Y– structures with Cs point-group
symmetry, and the front-side attack saddle points have either Cs (X = F or X = Y) or C1 symmetry with XCY angles in the 78–88°
range. On the basis of the previous reaction dynamics simulations
and the minimum energy path computations along the inversion coordinate
of selected XH···CH2Y– systems, we suggest that the double inversion may be a general mechanism
for SN2 reactions.