A R T I C L E S
Song et al.
Diels-Alder addition, which may explain the observation of
only this conformation. The 12 substituents on 6b largely project
away from the hexaphenylene core, which differs little from
the X-ray structure of the parent hydrocarbon 3,13 but the
substitution pattern gives rise to an unusual twisted, T-shaped
morphology with no large molecular cavity.
Computational Studies of Cyclic Oligophenylenes. We
were somewhat disappointed to obtain the screw isomer 6b,
for it is the crown isomer 5b that contains a large cavity formed
by the “crowning” phenyls. Might 6b be converted to 5b?
Aromatic hydrocarbons are relatively stable compounds, and
high temperatures could be employed for the isomerization. For
this reason, we used computational methods to examine the
interconversion of hexaphenylene atropisomers, a process that
seems not to have been considered previously by theorists.
Two questions must be asked. First, which of the isomers in
each pair is more stable, and second, what is the barrier to
interconversion? We examined the isomeric pairs 2 and 3 and
5b and 6b at four levels of theory (Table 1).11 At all levels, the
crown isomer 2 is more stable than 3, but the difference drops
from an estimated 22.1 kcal/mol by molecular mechanics
(MMFF) to 6.1 kcal/mol by density functional theory (B3LYP/
6-31G(d)14). In contrast, the results for 5b and 6b are scattered,
but the higher level calculations favor 6b by 4-5 kcal/mol. No
doubt the steric strain from colliding substituents at carbons 1,
4, 9, 12, 17, and 20 (the “equatorial” sites) in 5b nearly balances
the face-to-face repulsion of the benzene rings in 6b, and even
relatively high levels of theory can have difficulties assessing
nonbonded interactions accurately.15 Notably, in the case of the
dodecaphenylhexaphenylenes 5a and 6a, the screw isomer is
strongly favored: the “equatorial” phenyls are simply too
crowded in the crown isomer.
The question of interconversion is more difficult. In Wittig’s
original work,9 compound 2 was heated at 480 °C for 24 h
without detectable conversion to 3, and 3 was heated at 470 °C
for 8 h without conversion to 2! (Some decomposition was
observed in both cases, of course.) We examined the intercon-
version at both the AM116 and HF/3-21G17 levels of theory.
Extensive searches for any intermediates in the interconversion
were unsuccessful. Instead, only a single bona fide transition
state (16) was located at each level of theory,11 and small
perturbations to these structures cause them to evolve smoothly
to either 2 or 3 upon optimization. At the AM1 level, the
transition state is more than 90 kcal/mol above the ground state
2 and 71 kcal/mol above 3; at HF/3-21G, these values increase
to a daunting 109 and 97 kcal/mol! The two calculated transition
states are similar; both have C2 symmetry, and they result from
pulling two adjacent phenylene groups past each other. The HF/
Figure 1. Two views of the molecular structure of compound 6b. Thermal
ellipsoids are drawn at the 50% probability level, and hydrogen atoms have
been omitted for clarity.
and the desired triple Diels-Alder adduct were observed. The
mass spectrum of the monoadduct fraction exhibited a prominent
molecular ion at m/z 534, corresponding to the Bergman
cyclization product 15. An exact mass measurement confirmed
the formula as C42H30. However, this same material had very
1
complex H and 13C NMR spectra; the 19 strong peaks in the
13C NMR spectrum are consistent with the Cs-symmetric
structure 15, but a more complex, less intense subspectrum
indicated that a less symmetric isomer is also present.
The triple adduct from the reaction of 12 and 13 showed a
fast-atom bombardment (FAB) MS molecular ion at m/z 997
(12C7713CH60), as expected for a hexaphenylhexamethylhexa-
phenylene. However, hexaphenylenes may exist in either a
“crown” conformation (2 and 5, Chart 1) or a “screw” confor-
mation (3 and 6), which do not interconvert under normal
conditions.9 The 1H NMR spectrum of the triple adduct showed
three methyl resonances, the number expected for the C2-
symmetric screw isomer 6b (see Table 1), and the X-ray
structure (Figure 1) confirms that assignment. Indeed, the
molecule lies on a special position in the X-ray structure and
possesses crystallographic C2 symmetry.
(11) Molecular mechanics (MMFF) and semiempirical molecular orbital (AM1)
calculations were performed by using SPARTAN 5.0, and ab initio (HF/
3-21G) and density functional (B3LYP/6-31G(d)) calculations were
performed by using GAUSSIAN 98. In both programs, the default
thresholds for wave function and gradient convergence were employed.
Transition states were located by using the QST3 option in GAUSSIAN
98, and they were verified by analytical frequency calculations.
(12) Halgren, T. A. J. Comput. Chem. 1996, 17, 490-519.
For hexaphenylene itself, the crown isomer 2 is thought to
be more stable than the screw isomer 3, but both are formed in
each of the two literature syntheses of hexaphenylene.9,10
However, MMFF calculations11,12 suggest that the immediate
precursor of 6b, a double adduct of 13 to 12, strongly prefers
a C2 conformation that would lead directly to 6b upon the third
(13) Irngartinger, H. Acta Crystallogr., Sect. B 1973, 29, 894-902.
(14) (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. (c) Miehlich, B.; Savin,
A.; Stoll, H.; Preuss, H. Chem. Phys. Lett. 1989, 157, 200-206.
(15) (a) Pascal, R. A., Jr. J. Phys. Chem. A 2001, 105, 9040-9048. (b) Pascal,
R. A., Jr.; Hayashi, N.; Ho, D. M. Tetrahedron 2001, 57, 3549-3555.
(16) Dewar, M. J. S.; Zoebisch, E. G.; Healy, E. F.; Stewart, J. J. P. J. Am.
Chem. Soc. 1985, 107, 3902-3909.
(9) Wittig, G.; Ru¨mpler, K.-D. Liebigs Ann. Chem. 1971, 751, 1-16.
(10) Simhai, N.; Iverson, C. N.; Edelbach, B. L.; Jones, W. D. Organometallics
2001, 20, 2759-2766.
(17) Hehre, W. J.; Radom, L.; Schleyer, P. v. R.; Pople, J. A. Ab Initio Molecular
Orbital Theory; John Wiley & Sons: New York, 1986; pp 63-100.
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13734 J. AM. CHEM. SOC. VOL. 127, NO. 39, 2005