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of 2,2-disubstituted vinyl silanes can undergo desilylation to obtain 1,1-
disubstituted terminal epoxides [64].
Two extreme epoxidation transition states - spiro and planar - have been pro-
posed for the epoxidation with dioxiranes (Figure 15.4). Both experimental and
computational studies suggest that the spiro transition state is energetically favored
due to a stabilizing secondary orbital interaction between the nonbonding orbital
of the dioxirane oxygen and the
* orbital of the olefin [3, 4, 17, 46, 47, 65-72].
Studies have also shown that spiro transition state
A
is favored for the epoxidations
of
trans
- and trisubstituted olefins with ketone
1
based on the obtained epoxide
configurations (Figure 15.5). The stereochemical outcome of the epoxidation
reveals that planar transition state
B
is competing and that the competition is
dependent upon the steric and electronic nature of the olefin substituents [46, 47].
Generally speaking, conjugating aromatic rings, alkenes, and alkynes to the react-
ing double bond enhances the aforementioned secondary orbital interaction, thus
favoring spiro
A
over planar
B,
which leads to an increase in the enantioselectivity
of the resulting epoxide. A small R
1
group and/or a large R
3
group is also beneficial
for the enantioselectivity by sterically favoring spiro
A
and/or disfavoring planar
B.
The transition state model is validated by the results of kinetic resolution of
π
Figure 15.4
Spiro and planar transition states for the dioxirane epoxidation of olefins.
Figure 15.5
Competing spiro and planar transition states for the epoxidation with ketone
1.
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