Table 1 Energy differences (kcal molꢀ1), bond lengths for the newly
formed bond (A) and transition state frequencies (cmꢀ1) for the crucial
transition states shown in Fig. 2
In conclusion, we presented a comprehensive explanation
for the highly regioselective Scholl reaction leading to the
formation of tribenzo[fg,ij,rst]pentaphene derivatives by joint
experimental and quantum chemical investigations. Also, the
successful isolation of unprecedented mono-functionalised
tribenzo-[fg,ij,rst]pentaphene derivatives will be useful to eval-
uate future syntheses of oligoarene and graphene materials via
a Scholl reaction for unsymmetrical starting materials in the
synthesis of complex polyarene architectures.
TSA-B1X
TSA-B2X
r(C–C) nTS
r(C–C) nTS
X
DEa,b DEa,c DGa,b
H
F
2.8
4.8
0.7
2.6
5.3
2.0
4.2
5.3
1.781
1.729
1.775
ꢀ495 1.798
ꢀ589
ꢀ497 1.772
ꢀ531
OMe 6.1
ꢀ488 1.771
ꢀ523
E/G(TSA-B2X).
a
(Free) energy difference: E/G(TSA-B1X)
c
LC-oPBE/def2-SVP. B3LYP/def2-TZVPP//LC-oPBE/def2-SVP.
ꢀ
b
Notes and references
1 R. Scholl and J. Mansfeld, Ber. Dtsch. Chem. Ges., 1910, 43, 1734;
P. Kovacic and M. B. Jones, Chem. Rev., 1987, 87, 357.
barriers towards the experimentally observed product D1X (via
radical cation C1X) are favoured for all substituents X.
The free energy differences G(TSA-B1X) ꢀ G(TSA-B2X)
are 2.0 kcal molꢀ1 (X = H), 4.2 kcal molꢀ1 (X = F) and
5.3 kcal molꢀ1 (X = OMe) which are in line with the
experimentally observed high regioselectivity of the Scholl
reaction. Note that the calculated transition states exhibit
antarafacial arrangements of the aromatic rings. An alternative
suprafacial arrangement possesses transition states which are
5–10 kcal molꢀ1 higher in energy. Therefore, they are not
further discussed (details can be found in the ESIw).
The calculations indicate that the transition states lead to
energetically high lying intermediates B1X and B2X for all
substituents. We conclude that the intermediates are instanta-
neously deprotonated by chloride anions which are available
in solution forming HCl. Indeed, HCl has been experimentally
observed, confirming this assumption. The final product
regioisomer D1X is then formed via radical cation C1X in a
third electrocyclic reaction, in accordance with the experiment.
The energy differences for the crucial transition states are
consistent for both density functionals applied and range
between 0.8 and 6.1 kcal molꢀ1 (Table 1). The same holds
true for the difference in free energies. Thus for all substituents
a clear kinetic preference for the experimentally observed
pathway is found.
2 M. Klussmann and D. Sureshkumar, Synthesis, 2011, 353; A. A.
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9 In the case of FG=CH3 the methyl groups disappear and in
1H NMR olefinic protons can be detected.
10 O. Hammerich, in Organic Electrochemistry, ed. H. Lund and
O. Hammerich, Dekker, New York, 2001, ch. 13, p. 471.
11 When AlCl3 or MeSO3H was applied in the absence of an oxidizing
agent no conversion was observed.
In the analysis of the crucial transition states we found that
the preference for the pathway via TSA-B1X can be understood
in terms of frontier orbital analysis. Fig. 2 shows the LUMO of
12 L. Zhai, R. Shukla, S. H. Wadumethrige and R. Rathore, J. Org.
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AH and AF (AOMe looks similar). Upon inspection of the orbital
coefficients it can be seen that the coefficients at the central
aromatic ring are distributed unevenly. For all substitution
patterns, the carbon atoms being attacked through pathway c
(Scheme 5, AH) or g (Scheme 6, AF) exhibit the larger orbital
coefficients.
13 P. J. Donoghue and O. Wiest, Chem.–Eur. J., 2006, 12, 7019.
14 L. Zhai, R. Shukla and R. Rathore, Org. Lett., 2009, 11, 3474;
T. S. Navale, K. Thakur and R. Rathore, Org. Lett., 2011, 13, 1634.
15 The product was accompanied by an unidentified side-product.
16 Note that the transition states TSA-B1X could only be located with
the functional LC-oPBE. Previous attempts with B3LYP, BP86,
M06-2X, B97D and TPSS failed to locate a stationary point. The
observation that the identification of intermediates depends on the
method employed in radical cation reactions has been found earlier
(see ref. 13). Extensive benchmark studies on present day density
functionals (L. Goerigk and S. Grimme, Phys. Chem. Chem. Phys.,
2011, 13, 6670) reveal that care has to be taken in choosing the right
functional and basis set for studies in organic chemistry similar to
more challenging transition-metal catalyzed reactions. Although for
pericyclic reactions B3LYP has been found to provide reasonably
accurate results (T. Schwabe and S. Grimme, Acc. Chem. Res., 2008,
41, 569) excellent agreement with higher level calculations has been
found for radical cation reactions. (U. Haberl, O. Wiest and
E. Steckhan, J. Am. Chem. Soc., 1999, 121, 6730.) For further
details see the ESI.w In accordance with earlier observations (ref. 13
and therein), a non-aromatic to slightly antiaromatic character of
the transition states has been found by NICS computations.
It follows that the observed reactivity pattern is in line with
an orbital controlled reaction which may be used as an easy
probe for future studies on regioselective Scholl reactions.
Fig. 2 Lowest unoccupied orbital (LUMO) for AH (left) and AF
(right) with orbital energies (B3LYP/def2-TZVPP).
c
This journal is The Royal Society of Chemistry 2012
Chem. Commun., 2012, 48, 377–379 379