Fig. 2 Calculated lowest energy structure of dimer 3ÀÁ3À as obtained
from a force field calculation (Macromodel V 8.0, amber* force field,
GBSA solvation model).
X-ray crystal analyses reveal completely planar dimers at least
in the solid state, the dimer 3ÀÁ3À is slightly tilted. This could
however also be an artefact of the calculation as force field
calculations tend to overestimate stacking interactions. The
most likely explanation for the surprisingly high stability of
dimer 3ÀÁ3À is the fact that charged H-bonds are more stable
than neutral ones.8 Whereas within dimer 2Á2 all H-bonds are
formed between neutral H-bond donors and acceptors, within
3ÀÁ3À the H-bond acceptor (the carboxylate) is charged and
the two donors (the imido and the pyrrole NH, respectively)
are neutral. Of course even more stable dimers result when
also the H-bond donors are charged as in 1Á1. However, the
additional benefit of at least one charged H-bond not only
overcomes the mutual repulsion of the two anions but also
leads to significantly more stable self-assembly than in a
completely neutral H-bonded system. Long ranging charge
repulsion between the two interaction anions is most likely
also attenuated by the rather polar solvent.
Fig. 1 NMR dilution study of 3À (Na+-salt) in CDCl3/[d6]DMSO
1 : 1 (v/v). Shown is the shift change of the pyrrole NH along with the
non linear curve fit (red) which provides an association constant for
dimerisation of Kass = 145 MÀ1
.
the benzyl ester (H2/Pd/C in MeOH) in 7 the imidopyrrole
carboxylic acid 3 was obtained.
Similar to the previously studied knock-out analogue 2,4
the imidopyrrole carboxylic acid 3 did not show any signs of
self-assembly in pure DMSO solution (as judged by the
absence of any concentration dependent NMR shift changes).
Unfortunately, 3 is not soluble enough to study its self-
assembly in less polar solvents (e.g. CHCl3/DMSO mixtures).
However, the sodium salt of 3 is well soluble in a 1 : 1-mixture
of CHCl3/DMSO (v/v) and forms surprisingly stable dimers.
Dimerization was studied by following the 1H NMR shift
changes of either the methyl group CH3 protons or the pyrrole
NH proton upon dilution in the concentration range between
18 and 0.05 mM.6 Identical binding isotherms were obtained
which can be analyzed using non-linear regression. A dimeri-
zation constant of either Kass = 115 MÀ1 (CH3) or 145 MÀ1
(pyrrole NH) was obtained (Fig. 1), respectively (estimated
error in each K-value is ca. Æ20%). Hence, an average dimer
stability of ca. 130 MÀ1 results from the 1H NMR dilution
studies. To assure that the countercation does not affect the
dimerization, we also prepared the cesium salt of 3 and
performed the same dilution experiment (see ESIw). The shifts
are identical to those of the sodium salt and an identical
dimerization constant of Kass = 115 MÀ1 is obtained. Hence,
the presence of close ion pairs in these solvent mixtures or a
significant impact of the countercation on the dimerization
process are rather unlikely.
In conclusion we have shown here that the use of charge
assisted H-bonds is superior to neutral H-bonds to obtain
stable self-assembly in polar solution. Hence, for the design of
new self-complementary binding motifs not only the number
of H-bonds but even more importantly their nature (ion
paired, charged, neutral) should be taken into consideration.
Notes and references
1 (a) H.-J. Schneider and A. Yatsimirsky, Principles and Methods in
Supramolecular Chemistry, VCH, Weinheim, 2000; (b) J. W. Steed
and J. L. Atwood, Supramolecular Chemistry, Wiley, Chichester,
2000; (c) J.-M. Lehn, Supramolecular Chemistry: Concepts and
Perspectives, VCH, Weinheim, 1995.
2 (a) T. Rehm and C. Schmuck, Chem. Commun., 2008, 801–813;
(b) T. Rehm and C. Schmuck, Chem. Soc. Rev., 2010, 39,
3597–3611.
The dimer of anion 3À is therefore significantly more stable
than that of the neutral analogue 2 which in the same solvent is
at least one order of magnitude less stable (Kass o 10 MÀ1
already in 5% DMSO in CHCl3). This is quite surprising at the
first glance as the dimer 2Á2 is held together by a network of six
H-bonds whereas within dimer 3ÀÁ3À only four H-bonds are
possible. Furthermore, dimerization requires the interaction of
two anions. Nevertheless, the latter dimer is definitely more stable
than the former. Empirical force field calculations (Macromodel
V 8.0,7 amber* force field, water GBSA/solvation model)
confirm the possibility for anion 3À to form a dimer held
together by four H-bonds. The energy minimized structure is
shown in Fig. 2. In contrast to dimer 1Á1 or 2Á2, for which
3 Two recent reviews on the challenge of bringing supramolecular
chemistry into water can be found in: (a) G. V. Oshovsky,
D. N. Reinhoudt and W. Verboom, Angew. Chem., Int. Ed., 2007,
46, 2366–2393; (b) S. Kubik, C. Reyheller and S. Stuewe, J. Inclusion
Phenom. Macrocyclic Chem., 2005, 52, 137–187.
4 C. Schmuck and W. Wienand, J. Am. Chem. Soc., 2003, 125,
452–459.
5 (a) S. Schlund, C. Schmuck and B. Engels, J. Am. Chem. Soc., 2008,
127, 11115–11124; (b) C. Rether, W. Sicking, R. Boese and
C. Schmuck, Beilstein J. Org. Chem., 2010, 6, No. 3.
6 K. A. Connors, Binding Constants, John Wiley & Sons, 1987.
7 F. Mohamadi, N. G. J. Richards, W. C. Guida, R. Liskamp,
M. Lipton, C. Caufiled, G. Chang, T. Hendrickson and
W. C. Still, J. Comput. Chem., 1990, 11, 440–467.
8 (a) M. Meot-Ner, Chem. Rev., 2005, 105, 213–284;
(b) H.-J. Schneider, Angew. Chem., Int. Ed., 2009, 48, 3924–3977.
c
This journal is The Royal Society of Chemistry 2011
Chem. Commun., 2011, 47, 9078–9079 9079