ꢀꢀꢀꢁ
52ꢀ ꢀD. McTush-Camp et al.: Reaction of dimethyldioxirane with 1,3-cyclohexadiene and 1,3-cyclooctadiene
conformations were checked and corrected for conformational dif-
ferences, if present. For 2b, this was a problem that was solved
by constraining the conformation of the starting material during
the transition-state calculation. All calculations were completed
in the gas phase at 23°C for this study. The electronic activation
energies were calculated as follows: Eelect ꢀ=ꢀ energy of transition
state–(ground-state energy of dioxirane+ground-state energy of
substrate). To calculate the relative reactivities, the difference in the
rapidly and mixed (∼4 s) via pipette. The disappearance of dimethyl-
dioxirane was monitored vs. time at 330 nm for at least two half-lives.
For 1,3-cyclooctadiene, pseudo-first-order conditions were employed
with the diene concentration at least tenfold greater than that of 1.
For the more reactive 1,3-cyclohexadiene, second-order conditions
were employed. The k2 values were the average of at least three exper-
iments. All kinetic runs had correlation coefficients of 0.99 or greater.
Afer completion of each kinetic run, formation of the monoepoxide
was confirmed by GC-MS analysis.
electronic activation energies was used (Arrhenius equation) in the
-∆Eelect
following manner: k2rel =( e(
/RT ) )( k2normalized). The substrate
with the lower reactivity is normalized to 1. Inclusion of a solvent
in calculations, while affecting the individual values, did not affect
the electronic activation energy differences, in agreement with the
literature [18]. Therefore, all calculations were completed in the gas
phase at 23°C for this study.
Computational methodology
All calculations (gas phase) reported in this paper were per-
formed with the Spartan’10 molecular modeling program. The DFT
approach using Becke3-LYP and the 6-31 G basis set was utilized for
all calculations. Energies for the minimized ground-state structures
were determined for all the reactants [dimethyldioxirane (1), cyclic
dienes (2a and 2b), and the phenyl-substituted alkenes (4a and
4b)] and the products [acetone, corresponding monoepoxides (3a
and 3b), and epoxides (5a and 5b)]. As expected, the computational
data predicted that the reactions are exothermic in all cases. The
optimized ground-state energy structure of 1,3-cyclohexadiene was
predicted to be a relatively flat s-cis system. The optimized ground-
state energy structure of 1,3-cyclooctadiene is consistent with the
two double bonds not in the same plane with a torsion angle of
51°. The HOMO-LUMO energies were obtained from the optimized
geometries using the DFT approach using Becke3-LYP and the 6-31 G
basis set. As expected, the optimized transition state for each diene
resulted in a spiro-orientation with a slight asynchronous tilt away
from the other double bond of the cyclic system. Regardless of the
initial approach of the dioxirane, all valid transition states resulted
in the spiro-orientation. To save time, the calculations were carried
out with the methyl groups of the dioxirane oriented away from the
most hindered side of the diene, which always yielded the lowest
energy spiro-transition state. Each transition-state calculation was
checked for validity. A valid transition state had only one negative
eigenvalue, which also corresponded to the eigenvector in a sepa-
rate intrinsic reaction coordinate (IRC) calculation. When animated,
the IRC linked the starting materials to the desired products through
the spiro-oriented transition state. For the cyclic dienes, two reac-
tion sites are present and can be approached from the top or bot-
tom, yielding different outcomes due to conformational factors.
Because 1,3-cyclohexadiene is relatively flat, the transition states for
all approaches for monoepoxidation are of similar reactivity. Alter-
natively, for 1,3-cyclooctadiene, conformation is a major factor. All
approaches to the reaction sites were calculated. Due to significant
energy differences, one of the approaches was found to have a sub-
stantially lower electronic activation energy and therefore was the
major contributor to the overall reactivity for that case. Weighted
averages of the electronic activation energies for all orientations of
attack of 1 on the other substrates were not necessary. For the other
cases, the lowest electronic activation energy was taken as repre-
sentative. As shown for simple cis-alkenes [5], the approach to cis-
1-phenylpropene is with the methyl groups of the dioxirane away
from the hindered side. For the trans-1-phenylpropene, the transi-
tion state with the lowest energy is with the methyl groups of the
Acknowledgments: Acknowledgment is made to the US
Department of Education (GAANN Fellowship to Davita
McTush-Camp) and to the Georgia State University Depart-
ment of Chemistry. We would like to thank Dr. Navarro-
Einsenstein for help with the product studies.
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