RESUMEN
Systematic computational studies of pericyclic Diels-Alder reactions between (H3C)2C=C(CH3)2, 1, and all permutations of substituted cyclopentadienes c-C5R1R2R3R4R5aR5b (R = H, CH3, CF3, F) allowed isolation of substitutional effects on Gibbs free energy barrier heights and reaction Gibbs free energies. "Average Substitution Gibbs Free Energy Correction" ΔG ASC# /ΔG ASC# values for each substituent in each position appeared to be additive. Substituent effects on barriers showed interesting contrasts. Methyl substitution at positions 5a and 5b increased barriers significantly, while substitution at all other positions had essentially no impact. In contrast, fluoro substitution at positions 5a and 5b lowered barriers more than substitution at other positions. Trifluoromethyl substitution mixed these effects, in that substitution at positions 5a and 5b increased barriers, but substitution at other positions lowered them. Despite the variances, ΔG ASC# /ΔG ASC# values allowed reliable prediction of barriers and exergonicities for reactions between 1 and highly substituted cyclopentadienes, and between 1 and cyclopentadienes with random mixtures of CH3/CF3/F substituents. ΔG ASC# /ΔG ASC# values were correlated with steric considerations and quantum theory of atoms in molecules (QTAIM) calculations. Overall, the ASC values provide a resource for predicting which Diels-Alder reactions of this type should occur at rapid rates and/or give stable bicyclic products.
RESUMEN
Systematic computational studies of pericyclic Diels-Alder-type reactions between aminoborane (F3C)2B = N(CH3)2, 1, and all permutations of substituted cyclopentadienes c-C5R1R2R3R4R5aR5b (R = H, CH3, CF3, F) allow isolation of substitutional effects on Gibbs free energy barrier heights and reaction Gibbs free energies. The effects appear to be additive in all cases. Substitution at positions 5a and 5b always increases barriers and reaction energies, an effect explained by steric interactions between substituents and the aminoborane moiety. For cases R = CH3, regioselectivities differ from those expected from canonical organic chemistry predictions. Frontier molecular orbital calculations suggest this arises from the extreme polarization of the π interaction in 1. For cases R = CF3, the 2/3-substitution comparison accords with canon, but the 1/4-substitution comparison does not. This appears to arise from a combination of electronic and steric issues. For cases R = F, many of the reactions are exergonic, in contrast to the cases R = CH3, CF3. Additionally, fluorine substitution at positions 2 and 4 has a barrier-lowering effect. Frontier molecular orbital calculations support an orbital-based preference for formation of 2- and 4-substituted "meta" products rather than "ortho/para" products.
RESUMEN
Systematic computational studies of concerted pericyclic ene-type reactions between aminoborane (F3C)2B[double bond, length as m-dash]N(CH3)2, 1, and substituted propenes (R1a)(R1e)C[double bond, length as m-dash]C(R2)-C(R3a)(R3e)H (R = Me, CF3, F; a = axial position in transition state, e = equatorial position in transition state) show that in all cases but one the reactions are exothermic. The reactions proceed through six-membered cyclic envelope-like transition states except in the case of 1 + C3H(CF3)5. The data allow isolation of substitutional effects on barrier heights; the effects appear to be additive in all cases. Substitution at positions 1a, 1e, and 3a increases barriers, while substitution at positions 2 and 3e has variable impacts. The former observation is ascribed to steric crowding in the transition states, and is particularly prevalent for substitution at positions 1a and 1e. Substitution at position 2 lowers barriers for R = Me, F, possibly due to electronic demands, while raising them for R = CF3 because of 1,3-diaxial repulsions between boron- and carbon-bound CF3 groups. Substitution at position 3e has little impact on the barriers for R = Me, CF3, but significantly raises them for R = F. This seems to arise from charge effects on the position of the transition states.