DOI: 10.1002/chem.201603389
Communication
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Reaction Mechanisms
Azulene–Naphthalene-Type Rearrangements in Benz[a]azulene
and Cyclohepta[b]indole
Curt Wentrup*[a] and Jꢀrgen Becker[b]
ysis of 4–13C-azulene at 11808C/10ꢀ3 hPa (Scheme 1);[7] and 2)
Abstract: Flash vacuum pyrolysis (FVP) of benz[a]azulene
the 9,10-diradical mechanism of Scott and Kirms based on py-
yields phenanthrene and 2-ethynylbiphenyl. FVP of cyclo-
rolysis of 1–13C-azulene in an N2 flow system at 700–9008C
hepta[b]indole similarly yields phenanthridine and 2-cya-
with contact times of 0.3–3 min (Scheme 2).[8,9] A previously
nobiphenyl. The reversibility of the reactions is demon-
proposed pericyclic bicyclobutane mechanism[10] has been dis-
strated by FVP of 2-ethynylbiphenyl and 2-isocyanobi-
counted because of the high calculated activation barri-
phenyl. All the observed reactions are in accord with the
er,[5,6,11,12] and because it cannot account for most labeling re-
norcaradiene–vinylidene mechanism of the azulene–naph-
sults.[13]
thalene rearrangement, whereas other proposed mecha-
In addition, two intermolecular mechanisms involving the
nisms are ruled out.
addition of hydrogen atoms (or methyl radicals)—the methyl-
ene walk and spiran pathways—(Scheme 3) have been put for-
ward and promoted strongly by Alder and co-workers,[12] but
Introduction
suffer from the fact that none of the numerous postulated in-
termediates have ever been observed. The methylene walk
process allows the migration of a CH2 group from the seven-
to the five-membered ring (9!10). In the spiran route,
a carbon migration in the spirocyclic intermediate, 11!12,
and a 1,5-H shift 13!14 are required to turn a 2-subsituted
azulene into a 1-substituted naphthalene.
The thermal isomerization of azulene to naphthalene (A–N re-
arrangement) [Eq. (1)] has intrigued organic, physical and com-
putational chemists for nearly 70 years.[1] Although the reaction
is usually achieved by high-temperature flash, flow, or static
pyrolysis, recent variations include the graphite-sensitized, mi-
crowave-induced rearrangement[2] and a room temperature
cationic reaction promoted by BF3·Et2O.[3]
The mechanisms in Scheme 3 were developed largely to ex-
plain the rerrangements of methyl-substituted azulenes, for ex-
ample the fact that 2-[13C-methyl]-2–13C-azulene affords both
2-[13C-methyl]-2–13C-naphthalene and 1-[13C-methyl]-1–13C-azu-
lene (sealed tube, 4408C, 4 h),[12,14] but they ignore the fact
that azulene itself undergoes skeletal rearrangements under
these reaction conditions as summarized in Scheme 4.[15] For
example, 1-phenyl-1–13C-azulene isomerizes to 2-phenyl-2–13C-
azulene, and 1-phenyl-3–13C-azulene isomerizes to 2-phenyl-3a-
13C-azulene, whereas labels and substituents in the seven-
membered ring remain in their original positions.
The best available activation energy for the thermal A–N re-
arrangement, determined in shock tube experiments at 1000–
16008C with azulene highly diluted in Ar, is 63 kcalmolꢀ1 with
It has to be realized that no single mechanism for the A–N
rearrangement can explain all the experimental results,[7,16]
which is not surprising for a reaction taking place at tempera-
tures of 10008C or higher. Moreover, because of these extreme
conditions, authors often use poorer vacua (10ꢀ1–10ꢀ2 hPa) or
pack the pyrolysis tubes with quartz chips to increase the con-
tact times to seconds, or use higher pressure flow conditions
with contact times of minutes to lower the reaction tempera-
ture. Worse still, the reactions may be performed in sealed
tubes at for example 4008C for several hours.[12,14] It is no sur-
prise that multiple reactions, including radical-induced ones,
may take place under such conditions, and it is quite plausible
that the A–N rearrangement can be catalyzed by hydrogen
atom addition and elimination. We have shown that, under
FVP conditions with contact times in the millisecond range,
about 24% of intermolecular reaction occurs, as indicated by
the formation of [D0]naphthalene, [D1]naphthalene, and
an Arrhenius pre-exponential factor of 1012.93 [4]
.
Importantly, the
shock-tube reaction was found to be cleanly unimolecular.[4a]
A
somewhat higher activation energy of 73 kcalmolꢀ1 is predict-
ed by G3(MP2,CC) calculations,[5] whereas DFT calculations pre-
dict activation energies of 80 kcalmolꢀ1 or more.[6]
Two intramolecular mechanisms for the A–N rearrangement
have been proposed, 1) the norcaradiene–vinylidene mecha-
nism by Becker, Wentrup, Katz and Zeller based on flash pyrol-
[a] Prof. Dr. C. Wentrup
School of Chemistry and Molecular Biosciences
The University of Queensland, Brisbane, Qld 4072 (Australia)
[b] Dr. J. Becker
Fachbereich Chemie der Philipps-Universitꢀt
D-35037 Marburg (Germany)
Chem. Eur. J. 2016, 22, 1 – 6
1
ꢁ 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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