The atomic and group charges do not change from one
computational method to another. We conclude that the
polarization of the silyl group allows for favorable intra-
molecular stabilization of the carbanionic charge. Thus,
5-OSiR3 compounds react through a unique ring con-
formation in which the axial C-5 substituent effectively
blocks the cis face of the â-ketoester anion, directing the
electrophilic lead(IV) reagent more dramatically toward trans
product formation than would be expected through the
normal mechanism. Larger alkyl groups on the silicon
atom afford increasing blockage and selectivity (8 vs 1b)
until the size of the alkyl groups precludes close contact with
the anionic center. We believe that this is the origin of the
lower selectivity of 7, which bears the very large OTIPS
group.15
Table 2. Computed Conformational Energies for Anions 11
and 23a,b
carbanion calculation axial-endo axial-exo
equatorial
11
6-31+G(d,p)
B3LYP
0.00
0.00
0.00
0.00
0.00
0.00
0.00
0.00
-0.9
-0.2
+1.64
+1.12
-5.1
-5.0
-3.3
-4.0
MP2c
MP3//MP2d
6-31+G(d,p)
B3LYP
MP2c
MP3//MP2d
23
+1.3 (+4.4) -1.6 (+1.2)
+1.5 (+5.0) -0.94 (+2.4)
+5.8
+4.7
+2.4
+2.2
a Values are in kcal/mol. b Values in parentheses are for the MP2 wave
function computed at the optimized geometry for that row; i.e., MP2//RHF
or MP2//B3LYP. c Insufficient disk space to compute the MP2 frequencies;
the B3LYP values were used. d MP3 wave function calculated at the MP2/
6-31+G(d,p) geometry.
The delocalized nature of a â-ketoester anion is well-
known. However, charge must be localized on carbon at the
transition state for the reaction to proceed. Bernasconi and
Wenzel16 have shown that this localization of charge raises
the TS energy above that of the delocalized anion. We
interpret the MP3//MP2 results as a favorable interaction
between the diffuse silicon atom and the carbanion, providing
stabilization via orbital interactions that compensate for the
destabilization of the transition state due to charge localiza-
tion.
Our basic calculations13 (first two rows for each com-
pound) are consistent with positive A values7 for the silyloxy
and methoxy groups. The equatorial conformer in anion 23
is lower in energy by 1.6 kcal/mol (RHF) to 0.94 kcal/mol
(B3LYP); the observed value for a neutral system is 0.74
kcal/mol for -OSiMe3. These computed values are enthalpy
differences: ∆H ) ∆Eelec + ∆zpe + ∆CvibT with both the
zero-point energy (zpe) and vibrational heat capacity ap-
propriately scaled.14 HoweVer, the axial-endo conformation
in 23, with the silyloxy oriented toward the carbanion, is
the lowest in energy when the effects of polarization are fully
deVeloped in the Moller-Plesset method for electron cor-
relation. These effects are clearly evident at both the MP2
and MP3 levels of calculation. By contrast, the calculations
on the carbanion of 11 at this level show no change in the
dominant conformation.
In conclusion, aryllead(IV) tricarboxylates have been
shown to be effective arylation agents for the formation of
sp2-sp3 bonds with a variety of carbon acids. The present
study indicates that extremely high and predictable dia-
stereoselectivity (>99:1) in the formation of highly func-
tionalized quaternary centers can be achieved under mild
conditions, providing new opportunities for stereoselective
synthesis. Computational data suggest that the origin of this
selectivity is a stabilizing effect between the carbanionic
center of the â-ketoesters and a distal OSiR3 group. Further
studies with aryllead(IV) reagents are ongoing in our
laboratory and will be reported in due course.
Figure 1 depicts the computed axial-endo conformation
for both anions. For 11, the distance between the anionic
Acknowledgment. We wish to thank NSF (CDA-
9724237) for funding the purchase of computer facilities.
(13) Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb,
M. A.; Cheeseman, J. R.; Zakrzewski, V. G.; Montgomery, J. A., Jr.;
Stratmann, R. E.; Burant, J. C.; Dapprich, S.; Millam, J. M.; Daniels, A.
D.; Kudin, K. N.; Strain, M. C.; Farkas, O.; Tomasi, J.; Barone, V.; Cossi,
M.; Cammi, R.; Mennucci, B.; Pomelli, C.; Adamo, C.; Clifford, S.;
Ochterski, J.; Petersson, G. A.; Ayala, P. Y.; Cui, Q.; Morokuma, K.; Malick,
D. K.; Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Cioslowski, J.;
Ortiz, J. V.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz, P.; Komaromi,
I.; Gomperts, R.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham, M. A.;
Peng, C. Y.; Nanayakkara, A.; Gonzalez, C.; Challacombe, M.; Gill, P. M.
W.; Johnson, B. G.; Chen, W.; Wong, M. W.; Andres, J. L.; Head-Gordon,
M.; Replogle, E. S.; Pople, J. A. Gaussian 98, revision A.9; Gaussian,
Inc.: Pittsburgh, PA, 1998.
Figure 1. Calculated structures of the carbanions formed from 11
(left) and 23 (right) showing distances (Å) between the carbanionic
carbon and the methyl or silyl group. For 23, geometries around
the silicon atom are also given. (Carbon, gray; oxygen, red; silicon,
blue; hydrogen, white.)
(14) (a) Scott, A. P.; Radom, L. J. Phys. Chem. 1996, 100, 16502-
16513. (b) The enthalpy must be corrected for thermal effects to 298 K.
Since these calculations are relative to the center of mass, the vibrational
heat capacity is the only significant correction.
(15) For a review of the triisopropylsilyl group in organic chemistry,
see: Ru¨cher, C. Chem. ReV. 1995, 95, 1009-1064.
(16) (a) Bernasconi, C. F.; Wenzel, P. J. J. Am. Chem. Soc. 1994, 116,
5405-13. (b) Bernasconi, C. F.; Wenzel, P. J. J. Org. Chem. 2001, 66,
968-79.
center and the carbon of the C-5 substituent is invariant with
computational method. Anion 23, on the other hand, shows
significant variation in distance for the silicon atom to the
anionic center. In addition, the angles around the silicon atom
suggest partial rehybridization toward pentacoordinate ge-
ometry.
Org. Lett., Vol. 4, No. 23, 2002
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