Scheme 1
pathway in an Onsager continuum model for dimethylfor-
mamide (DMF)8 (∆G ) 25.8 kcal/mol) and occurs via a
concerted π-addition-elimination pathway in the gas phase
[B3LYP/6-31+G(d)] (Scheme 1).6 This mechanistic change
inspired us to do further study on the in-plane SN2 reaction.
All calculations were performed using the Gaussian 98
program.9,10
The transition structure for the cyclization of E-1b was
located in the gas phase and in solution by the B3LYP hybrid
functional13 together with the 6-31+G(d) basis and the
Onsager continuum model14 for DMF (ꢀ ) 37.06) (Figure
1). The in-plane SN2 transition structure E-1b-ts was obtained
with the activation free energy of 14.4 kcal/mol in DMF (17.1
kcal/mol in the gas phase). Hydrogen bonding of the
oxyanion with the vinylic hydrogen makes E-1b a planar
molecule. The intrinsic reaction coordinate (IRC) calculations
showed that spontaneous dissociation of the C-Cl bond
occurs when the oxyanion approaches the sp2 carbon while
Figure 1. Transition structures for the nucleophilic cyclization of
chloroalkene anions 1b and 3a [B3LYP/6-31+G(d), SCRF (dipole,
solv ) DMF)]. The italic numbers are the values in the gas phase.
keeping this hydrogen bonding (the O-H distance is 2.00-
2.23 Å). The distances of the forming O-C and the breaking
C-Cl bonds are 2.22 and 2.23 Å in E-1b-ts, respectively,
while the distance of the CdC double bond was slightly
reduced. Even after many trials, we could not get any
π-addition transition structures. On the other hand, only
π-addition transition structures are obtained from both Z-1b
and the dichloro compound 3a.6 Due to both the steric
hindrance and electronic repulsion between the oxyanion and
the electronegative chlorine atom, both Z-1b and 3a are no
longer planar molecules and the oxyanion approaches to the
sp2 carbon to the double bond plane perpendicularly. The
activation energies of these are much higher than the one of
E-1b. The high activation energies for the π-addition are
mainly associated with large deformation energies required
to adjust the reactants to their TS geometry without interac-
tion with the nucleophile. The deformation energy might be
roughly estimated by the energy difference (38.6 kcal/mol)
between Z-1b and Z-1b-ts, in both of which the alkoxy anion
was replaced with a hydrogen. Since the deformation energy
destabilizes the π-addition TS and the intramolecular hy-
drogen bonding stabilizes the in-plane SN2 type reaction,
E-1b-ts becomes the only favorable pathway. The in-plane
SN2 type reaction is also the preferred pathway for the
corresponding bromoalkene E-1c.15
(6) Ando, K. J. Org. Chem. 2004, 69, 4203-4209.
(7) Yanagisawa, H.; Miura, K.; Kitamura, M.; Narasaka, K.; Ando, K.
Bull. Chem. Soc. Jpn. 2003, 76, 2009-2026.
(8) Since DMF is able to dissolve many salts and tends to surround metal
cations rather than nucleopfilic anions, the use of free anions as model
systems could be approved.
(9) 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.; Baboul, A. G.; 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.; Challacombe, M.; Gill, P.
M. W.; Johnson, B.; Chen, W.; Wong, M. W.; Andres, J. L.; Gonzalez, C.;
Head-Gordon, M.; Replogle, E. S.; Pople, J. A. Gaussian 98, Revision A.9;
Gaussian, Inc., Pittsburgh, PA, 1998.
(10) Gibbs free energies are the values at 298.15 K and 1.00 atm. The
thermal energy corrections are not scaled.11 Vibrational frequency calcula-
tions gave only one imaginary frequency for all transition structures and
only harmonic frequencies for the reactants and products. The structures
of the reactants and products were obtained by the optimization of the last
structures on both sides of IRC calculations.12
(11) The scale factors for B3LYP are very close to 1.0; see: Bauschlicher,
C. W., Jr.; Partridge, H. J. Chem. Phys. 1995, 103, 1788-1791. Scott, A.
P.; Radom, L. J. Phys. Chem. 1996, 100, 16502-16513.
(12) (a) Gonzalez, C.; Schlegel, H. B. J. Chem. Phys. 1989, 90, 2154-
2161. (b) Gonzalez, C.; Schlegel, H. B. J. Phys. Chem. 1990, 94, 5523-
5527.
(13) (a) Becke, A. D. J. Chem. Phys. 1993, 98, 5648-5652. (b) Lee,
C.; Yang, W.: Parr, R. G. Phys. ReV. B 1988, 37, 785-789.
(14) (a) Onsager, L. J. Am. Chem. Soc. 1936, 58, 1486-1493. (b) Wong,
M. W.; Frisch, M. J.; Wiberg, K. B. J. Am. Chem. Soc. 1991, 113, 4776-
4782.
To see the effect of the benzene ring as a linker, the
cyclization reaction of the anion 4a was studied. The
transition structures for the cyclization of E-4a were located
(15) Full details will be soon presented.
2462
Org. Lett., Vol. 6, No. 14, 2004