internal position of the vinylallenes may play a role in the
regioselectivity.8
accurate energies. The nature of all the stationary points was
resolved through harmonic analysis. Solvent effects were
taken into account with sequential single-point calculations
at the gas-phase optimized geometries. A variation of the
conductor-like screening model (COSMO)14 method was
chosen (heptane) using the parameters proposed by Klamt.15
All the calculations were performed with the Gaussian 0316
suite of programs.
(b) Electron-withdrawing groups at the vinylallene termini
(CHO), on the other hand, inhibited the addition of SO2, and
vinylallenal 10 was recovered unchanged after 1 h at 25 °C
(at 80 °C, decomposition was observed). Electron-rich
divinylallene 11 suffered extensive decomposition under the
reaction conditions.
(c) (Z)-Vinylallenes are less reactive than the correspond-
ing E isomers. The structure of 14 confirms that the
cheletropic reaction occurred at the diene subunit of E
geometry despite being less substituted.
(d) Diastereoselectivity (or rotational selectivity on the
vinylallene) appears to be governed by steric factors. The
approach of the reagent from the less-hindered side of the
vinylallene dictates the disrotatory movement of the termini
(out,out in the enantiomers shown in Scheme 2), due to the
requirement of orbital overlap between the two reactants.
The allene axis configuration is thus transferred to the
exocyclic double-bond geometry (Scheme 3), and therefore
Transition structure geometries are highly asymmetric,
with sulfur-cumulene carbon bond lengths shorter (2.10-
2.27 Å) than the sulfur-olefin carbon counterparts (2.55-
2.69 Å). Small variations of these bond distances are
observed upon changes in the olefin geometry and the face
approach (syn/anti, see Scheme 3). Interestingly, the greatest
difference in forming bond lengths is observed with C3-
methyl-substituted vinylallenes. This effect, likely due to
back-strain, has also direct energetical implications, since
these substrates proceed through transition states that are
from 1 to 5 kcal/mol lower in energy than their unsubstituted
counterparts (see Table 1).
Scheme 3. Models of Computed Cheletropic Additions of SO2
Table 1. Gas Phase and Solution (COSMO, Heptane) Relative
Free Energies of Activation (kcal/mol, 298 K) of Models 1-4
to Vinylallenesa
gas phase
COSMO
syn
anti
syn
anti
(E)-r-1
(Z)-r-1
(E)-r-2
(Z)-r-2
(E)-r-3
(Z)-r-3
(E)-r-4
(Z)-r-4
27.37
34.15
26.33
29.06
27.54
30.37
31.03
33.97
26.63
33.59
25.10
28.40
25.47
28.78
26.55
30.61
26.38
33.04
24.42
27.28
25.63
28.33
29.25
32.82
24.99
31.99
22.79
26.05
23.63
26.89
24.18
28.88
a Note that the Z/E geometry of the olefin remains undefined in
the proposed nomenclature and will be specified along the discus-
sion.
Further inspection of Table 1 reveals the sources of
selectivity in the cheletropic additions. First, the Z geometry
of the vinyl moiety is a major contributor to the reaction
energetics. Transition structures of these isomers present even
more destabilization (2.83-6.96 kcal/mol) than that due to
allene substitution (1.45-4.91 kcal/mol). The trend of greater
if enantiopure reactants were used, the absolute configuration
of the sulfolene stereocenter would also be under the control
of the allene axial chirality.
To theoretically support the above findings and to get
further insight into the factors responsible for the regio- and
(14) Klamt, A.; Schu¨u¨rmann, G. J. Chem. Soc., Perkin Trans. 2 1993,
2, 799.
(15) Klamt, A.; Jonas, V.; Bu¨rger, T.; Lohrenz, J. C. W. J. Phys. Chem.
A 1998, 102, 5074.
the stereoselectivity, computations were carried out on
11,12
reactions of SO2
with model (E)- and (Z)-vinylallenes
(16) Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb,
M. A.; Cheeseman, J. R.; Montgomery, J. A., Jr.; Vreven, T.; Kudin, K.
N.; Burant, J. C.; Millam, J. M.; Iyengar, S. S.; Tomasi, J.; Barone, V.;
Mennucci, B.; Cossi, M.; Scalmani, G.; Rega, N.; Petersson, G. A.;
Nakatsuji, H.; Hada, M.; Ehara, M.; Toyota, K.; Fukuda, R.; Hasegawa, J.;
Ishida, M.; Nakajima, T.; Honda, Y.; Kitao, O.; Nakai, H.; Klene, M.; Li,
X.; Knox, J. E.; Hratchian, H. P.; Cross, J. B.; Adamo, C.; Jaramillo, J.;
Gomperts, R.; Stratmann, R. E.; Yazyev, O.; Austin, A. J.; Cammi, R.;
Pomelli, C.; Ochterski, J. W.; Ayala, P. Y.; Morokuma, K.; Voth, G. A.;
Salvador, P.; Dannenberg, J. J.; Zakrzewski, V. G.; Dapprich, S.; Daniels,
A. D.; Strain, M. C.; Farkas, O.; Malick, D. K.; Rabuck, A. D.;
Raghavachari, K.; Foresman, J. B.; Ortiz, J. V.; Cui, Q.; Baboul, A. G.;
Clifford, S.; Cioslowski, J.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz,
P.; Komaromi, I.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham, M. A.;
Peng, C. Y.; Nanayakkara, A.; Challacombe, M.; Gill, P. M. W.; Johnson,
B.; Chen, W.; Wong, M. W.; Gonzalez, C.; Pople, J. A. Gaussian 03,
revision B.02; Gaussian, Inc.: Pittsburgh, PA, 2003.
substituted at C1 and C5 (and C3). DFT was chosen due to
the satisfactory results reported in precedent studies with
dienes.13 The multilevel B3LYP/6-311++(3df,2p)//B3LYP/
6-31+(d,p) methodology was selected in order to obtain
(11) Kinetic studies revealed that the reaction of dienes is second order
in SO2, and in fact theoretical computations suggested a role for SO2 as a
Lewis acid.12 However regio- and diastereoselectivity are considered not
to be affected by the SO2 molecularity since the second SO2 molecule does
not modify the disrotatory nature of the reaction and merely acts as an
activating species for the reacting SO2 molecule.
(12) Ferna´ndez, T.; Sordo, J. A.; Monnat, F.; Deguin, B.; Vogel, P. J.
Am. Chem. Soc. 1998, 120, 13276.
(13) Monnat, F.; Vogel, P.; Rayo´n, V. M.; Sordo, J. A. J. Org. Chem.
2002, 67, 1882.
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