helical band found in diluted solution suffered a red shift
until 235 nm associated with the conformational change and
aggregation.
H-bonds and in consequence to lower stability of their folded
conformations. Nevertheless, transfer-NOE experiments on
those gels supported the partial unfolding of the molecule as
a general mechanism.
The observed evolution of the CD of concentrated mixtures
upon slow cooling suggested that an additional slow confor-
mational reorganization was taking place yielding a thermo-
stable gel (Scheme 2).z The higher degree of organization in
this gel is clearly supported by several facts. First, the WAXD
pattern of the xerogels obtained by slow cooling showed sharp
reflections denoting a high degree of crystallinity in the fibers
whereas that of the xerogel obtained after spontaneous
cooling gelation only showed a broad signal at 4.5 A and a
background of an amorphous material, in accordance with a
loosely defined aggregation as a result of the reduced number
on intermolecular interactions. This peak is typical for inter-
molecular distance in the H-bonding direction (see Fig. 3 and
ESIw) as described for analogues.4a Secondly, a kinetic study
of the aggregation under controlled cooling conditions at
35 1C revealed an activation free energy for the reorganization
process of 28 kJ molꢁ1 in agreement with the rupture of
several hydrogen bonds. Finally, the solubility of the gel
formed by 1a under kinetic conditions determined by
1H NMR was 12 mM whereas for the thermodynamic gel was
8 mM reflecting stronger intermolecular interactions and
increased gelation ability in the latter case.10 These properties
are related to the higher thermal stability measured for the gels
obtained by slow cooling (Tgel = 75 1C) as compared to the
kinetic gels (Tgel = 55 1C).
In summary, we have presented an example of small
peptidomimetics that evidence the paramount importance of
folding and aggregation even for a priori simple molecules. We
have shown that very subtle structural and environmental
changes may have a dramatic effect on supramolecular aggre-
gation. We have also proved that, upon overcoming the
required energy barrier these reversible supramolecular
systems are capable of self-correction to produce a more stable
and organised material. Current work is being done with
the aim of controlling the switching between soluble and
aggregated states.
We thank MEC (Grant CTQ2006-14984) and Universitat
Jaume I-Bancaixa (Grant P1ꢂ1A2006-1) for financial support.
F. R. Ll. thanks Generalitat Valenciana for a FPI fellowship.
Notes and references
z CD experiments of gels formed by fast cooling at different tempera-
tures (10, 0, ꢁ20 1C) confirmed the strong influence of cooling rate and
allowed the observation of kinetically trapped intermediate partially
unfolded conformations.
1 (a) Mechanisms of Protein Folding, ed. R. H. Pain, Oxford
University Press, 2000; (b) Self-assembling Peptide Systems in
Biology, Medicine and Engineering, eds. A. Aggeli, N. Boden and
S. Zhang, Kluwer, Dordrecht, 2001.
Very interestingly, a kinetically trapped gel was able to self-
correct when it was kept for 48 h at 30 1C being converted into
a gel with properties similar to those of the material obtained
by slow cooling (solubility and WAXD pattern of the xerogel).
Some differences were observed in the aggregation of com-
pounds 1b and 1c as compared to 1a. Firstly, spontaneous
cooling had to be employed in order to obtain gels whereas
slow cooling produced crystalline precipitates. On the other
hand, CD investigation of the aggregation process did not
reveal a strong influence of the cooling methodology as
described for compound 1a. Finally, WAXD of xerogels and
precipitates were identical (see ESI). Altogether these results
suggested that in these two compounds the energetic barrier
for conformational changes is much lower than for compound
1a probably related to the higher flexibility of the alkyl spacer
that, as already mentioned, led to weaker intramolecular
2 I. W. Hamley, Angew. Chem., Int. Ed., 2007, 46, 8128.
3 L. D. Estrada and C. Soto, Curr. Top. Med. Chem., 2007, 7, 115.
4 (a) B. Escuder, S. Martı and J. F. Miravet, Langmuir, 2005, 21,
´
6776; (b) J. F. Miravet and B. Escuder, Chem. Commun., 2005,
5796; (c) J. F. Miravet and B. Escuder, Org. Lett., 2005, 7, 4791.
5 (a) K. Hanabusa, R. Tanaka, M. Suzuki, M. Kimura and
H. Shirai, Adv. Mater., 1997, 9, 1095; (b) M. Doi, A. Asano,
H. Yoshida, M. Inouguchi, K. Iwanaga, M. Sasaki, Y. Katsuya,
T. Taniguchi and D. Yamamoto, J. Pept. Res., 2005, 66, 181.
6 V. Ottani, D. Martini, M. Franchi, A. Ruggeri and M. Raspanti,
Micron, 2002, 33, 587.
7 (a) Molecular Gels: Materials with Self-assembled Fibrillar Networks,
eds. P. Terech and R. G. Weiss, Springer, Dordrecht, The
Netherlands, 2006; (b) F. Fages, Top. Curr. Chem., 2005, 256, 1.
8 H. C. Ahn and K. Choi, Org. Lett., 2007, 9, 3853.
9 B. Escuder, M. Llusar and J. F. Miravet, J. Org. Chem., 2006, 71,
7747.
10 A. R. Hirst, I. A. Coates, T. R. Boucheteau, J. F. Miravet,
B. Escuder, V. Castelletto, I. W. Hamley and D. K. Smith,
J. Am. Chem. Soc., 2008, 130, 9113.
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