(such as 16) than it had been for trans-allyl sulfones (such
as 4) using Newman projections or Dreiding models failed
to provide a convincing explanation, we used a simple
molecular modeling approach to help guide us in the
formulation of a hypothesis. It has been suggested8 that there
are a number of accessible structures for solvated allyl
sulfone lithium species, including some in which the lithium
is remote from the reacting site. The metal ion and solvation
shell are thus less likely to dominate the reaction profile,
justifying a highly simplified model in which the cation and
solvent were ignored. Further support for this simplification
came from our experiments, which showed that the stereo-
chemical outcome of the cis-allyl sulfone cyclization was
essentially independent of the cation. Without detailed
knowledge of the solvation state and the location of the
cation, the conclusions from these studies must be seen as a
starting point for future, more detailed theoretical and
experimental investigations, but nonetheless provide some
support for an initial hypothesis as to the origin of the
observed stereocontrol. We initially considered the possibility
that the transition state would be starting-material-like and
studied the likely conformational preferences of the anion
of 16 and of the trans double-bond isomer of 16. A grid
search of the conformational energy was carried out on the
anionic species using the MMFF94S force field and charge
model in Sybyl.9 The C2-C1 bond was rotated 360° in 15°
increments and the C1-O bond rotated 360° in 60° incre-
ments. However, the conformational profiles of both cis- and
trans-allyl sulfone anions were very similar, with the lowest-
energy conformation in each case being one that would lead
to the cis-cyclopropane, with conformations that would give
rise to the trans-cyclopropane, higher in energy by ca. 2 kcal/
mol. Simplified structures (methyl instead of phenyl, and
methoxy instead of MOM) based on the local energy minima
located by MMFF were subjected to geometry optimization
at the ab initio HF/3-21G* level (using Spartan10) and showed
slightly decreased energy differences but the same general
trend (preference for the cis-cyclopropane precursor confor-
mation of 1.56 and 0.65 kcal/mol for the cis and trans double
bond, respectively, clearly not in line with observation). We
therefore considered the possibility that the transition state
was product-like and examined the conformations of the
product cyclopropanes 17 and 18. We constrained the C7-
C6-C2-C1 torsion to the eclipsed syn and anti positions,
modeling the expected initial product of the cis- and trans-
allyl sulfone cyclizations, respectively. The top two structures
in Figure 4 are models for product-like transition states of
trans-allyl sulfone cyclization, while those in the lower half
are models for the cyclization of the cis allyl sulfones. The
structures on the left are trans-cyclopropanes (conformers
of 17), and those on the right are cis-cyclopropanes (con-
formers of 18). In each case, the trans-cyclopropane is
slightly lower in MMFF94s energy. The difference is larger
for the bottom two structures in Figure 4, based on the cis-
allyl sulfone, than for the top two structures, albeit by only
Figure 4. Models for product-like transition states for trans- (top)
and cis- (bottom) allylsulfone cyclizations to trans- (left side) or
cis- (right side) cyclopropanes.
0.4 kcal/mol; this is consistent with a stronger preference
for trans-cyclopropane formation from the cis double-bond
precursor than from the trans double-bond precursor. As a
difference between energy differences, the 0.4 kcal/mol value
should benefit from cancellation of error and hence be a
useful indicator of the trend, despite its magnitude. Repetition
of the calculation at the ab initio HF/6-31G* level in Spartan
suggests that cyclization of the trans isomer of 16 should
preferentially give rise to the cis-cyclopropane (difference
of 0.87 kcal/mol), while cyclization of the cis compound 16
should preferentially give rise to the trans-cyclopropane
(difference 0.93 kcal/mol); hence, the difference between
energy differences at the HF/6-31G* level is widened to 1.8
kcal/mol. This appears to arise from an unfavorable interac-
tion between the proton on the C7 carbon and the oxygen
atom of the MOM group, as can be seen in the lower right
structure in Figure 4. This interaction would indeed be
expected to be significant in a late transition state for the
cyclization of 16 to the cis-cyclopropane 18 but is absent
for the trans product 17 or for trans-allyl sulfone starting
materials. Thus, it seems reasonable to suggest that the
stereochemical outcome of this reaction is due to a fairly
late transition state in which the unfavorable C7-O interac-
tion is avoided to give the trans-cyclopropane 17 as the major
product.
The versatility of vinyl sulfones in organic chemistry11 is
well-known, in particular as Michael acceptors and in
stabilization of an anion at the R-position.12 These com-
pounds seemed to us to be excellent starting materials to
explore the utility of lithiated Scho¨llkopf’s bislactim ether13
in Michael addition with vinyl sulfones. This methodology
has been widely employed in aldol reactions and Michael-
type reactions with ester, nitro, R,â-unsaturated 2,4-penta-
dienoates and 1,3-butadienylphosphonates.14
(11) (a) Ba¨ckvall, J.-E.; Juntunen, S. K. J. Org. Chem. 1988, 53, 2398.
(b) Fuchs, P. L.; Hentemann, M. F. Org. Lett. 1999, 1, 1355. Iradier, F.;
Arrayas, R. G.; Carretero, J. C. Org. Lett. 2001, 3, 2957. (c) Padwa, A.;
Murphree, S. S.; Ni, Z. J. J. Org. Chem. 1996, 61, 3829. (d) Ba¨ckvall,
J.-E.; Chinchilla, R.; Na´jera, C.; Yus, M. Chem. ReV. 1998, 98, 2291.(e)
Iradier, F.; Arrayas, R. G.; Carretero, J. C. Org. Lett. 2001, 3, 2957. (f)
Ba¨ckwall, J.-E.; Chinchilla, R.; Na´jera, C.; Yus, M. Chem. ReV. 1998, 98,
2291
(8) Piffl, M.; Weston, J.; Gu¨nther, W.; Anders, E. J. Org. Chem. 2000,
65, 5942
(9) Sybyl, version 6.9; Tripos, Inc.: St. Louis, MO.
(10) Spartan 02 Windows; Wavefunction, Inc.: Irvine, CA.
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