D. Trauner, M. Winkler, R. G. Bergman et al.
cyclization energy barriers increase for 6H relative to 6, we
believe that the transformation from 6H to product then
occurs on the thermal reaction pathway via 6 to 7 to 2
[
(
Chromenes) in Organic Photochromic and Thermochromic Com-
(
Scheme 3).
pounds, Vol. 1 (Eds.: J. C. Crano, R. Guglielmetti), Plenum Press:
New York, 1999, pp. 111–140; c) J. D. Hepworth, B. M. Heron,
Prog. Heterocycl. Chem. 2005, 17, 33–62; d) A. Samat, R. Gugliel-
metti, Chromogenic Materials, Photochromic in Kirk Othmer ency-
clopedia of chemical technology, Vol. 6, 5th ed. (Ed.: A. Seidel),
Interestingly, calculations indicate that the chromene
product is unstable towards protonation. The protonated
chromene 2H occupies a very flat minimum on the potential
energy surface and after inclusion of zero-point vibrational
energy corrections, the corresponding ring-opening transi-
tion state TS5H disappears as a stationary point, so that
ring-opening of the protonated chromene becomes barrier-
less. Once formed, however, the chromene product is pre-
sumably not basic enough to be protonated and is therefore
stable under the conditions used in our experiments.
In summary, we have provided evidence that the cycliza-
tion of E-configured vinyl o-QMs involves a relatively slow
acid-catalyzed exo-alkylidene bond isomerization followed
by faster oxa-6p electrocyclization. Computations indicate
that the overall reaction is catalyzed by Brønsted acids, but
the oxa-6p electrocyclization step itself is not prone to such
catalysis. The vinyl o-QM was found to be surprisingly basic,
allowing for quantitative protonation with relatively weak
acids. In addition, we have identified a new mode of Diels–
Alder dimerization of vinyl o-QMs. The factors determining
the stability of o-QMs towards dimerization are currently
under investigation in our laboratories.
[
[
5] R. W. Van De Water, T. R. R. Pettus, Tetrahedron 2002, 58, 5367–
405.
[
[
5
7] J. Sandstrom, Top. Stereochem. 1983, 14, 83–181.
[
[
8] The calculated dipole moments of TS1 and 1 are 4.56 and 4.52 D, re-
spectively. The intrinsic molecular charge distribution, as conjec-
tured from natural population analysis, is also comparable for both
stationary points. The strongly negative entropy of activation for the
E/Z isomerization step might be attributable to the fact that the
transition state is polar in all three spatial directions, whereas 1 is a
planar species, resulting in stronger solvation of the former. All cal-
culations have been carried out at the B3LYP/6-31G* level using
Gaussian 03: M. J. Frisch, et al. Gaussian 03; Gaussian, Inc.: Pitts-
burgh PA, 2003. See the Supporting Information for complete cita-
tion. All RDFT stationary points have been checked for triplet in-
stabilities by calculating the eigenvalues of the Hermitian stability
matrices. UDFT energies are reported throughout whenever an ex-
ternal instability was found.
Experimental Section
Experimental procedures, characterization data for products, and com-
plete citation of reference [8] are available in the Supporting Informa-
tion.
[
9] Kinetic data were not obtained for the thermal reaction at 218C.
This rate acceleration is based on extrapolation of the thermal
Eyring plot.
[
2
10] A kinetic isotope effect of 1 using ClCH COOD was measured
under acid-saturation; see Supporting Information.
11] From the available data it cannot be determined conclusively that
the enthalpy-entropy compensation effect observed is not simply a
result of the fact that the enthalpy and entropy are both derived
[12] Despite several attempts, TS1H could not be located as a stationary
point on the PES at the RB3LYP or UB3LYP level. Given the
almost identical energies of TS1 and TS4, and according to single
[
Acknowledgements
We are indebted to Dr Allen Oliver at the UC Berkeley CHEXRAY X-
ray crystallographic facility for X-ray crystal structure determinations
and Dr. Kathleen Durkin and Dr. Jamin Krinsky at the Molecular
Graphics Facility (NSF grant CHE-0233882). We acknowledge financial
support from NSF grant CHE-0345488 (to R.G.B.) and CHE-0548209 (to
K.N.H.). M.W. thanks the Alexander von Humboldt foundation for a
Feodor-Lynen fellowship and the Fonds der Chemischen Industrie for a
Liebig fellowship.
point energy calculations, the energy of TS1H relative to 1H is esti-
À1
mated to be 24–25 kcalmol
.
Keywords: activation parameters
·
alkenes
·
density
Received: April 8, 2008
functional calculations · dimerization · isomerization
Published online: April 30, 2008
5408
ꢀ 2008 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2008, 14, 5405 – 5408