supramolecular aggregations in solution, a double logarithmic
plot of specific viscosity versus concentration of monomer 3 in
CH3CN (see Figure S6 in the Supporting Information) was
obtained. In the low concentration range, the curve had a
slope of 1.02. As the concentration increased, the slope of the
curve approached 2.32. The linear relationship (slope of 1.02)
indicated the presence of noninteracting assemblies of a
constant size, whereas an exponential relationship (slope > 2)
is consistent with the presence of a supramolecular polymer-
ization process, in which the size of the resulting polymer
increased with concentration. The CPC for monomer 3 in
CH3CN was about 60 mm as evidenced by the clear change of
slope occurring at this concentration, indicating a ring–chain
transition from the formation of cyclic oligomers to highly
ordered polymers; hence, the mobility of the polymeric chains
is restricted.[1i,j,l,11]
Furthermore, rodlike fibers with a regular diameter of
8 mm were drawn from a high concentration solution and
observed by scanning electron microscopy (SEM), providing
direct evidence of the formation of supramolecular polymers
with high molecular weight and a high degree of linear chain
extension (see Figure 3a). Next, the gelation properties of the
synthesized monomer 3 were investigated (Figure 2). The
novel supramolecular polymer gel was prepared by dissolving
monomer 3 in CH3CN at 508C followed by cooling to room
temperature. Upon increasing the concentration of monomer
3 from 10 mm to 35 mm, the solution became a mixture of
solution and gel, and finally formed a gel at a phase-transition
temperature of approximately 408C; the critical gel concen-
tration was calculated to be 4.6 wt%.
acid. This process was also demonstrated by 1H NMR experi-
ments (see the Supporting Information) and SEM experi-
ments (see the Supporting Information). The addition of
20 mL of triethylamine to a solution of monomer 3 in
[D3]acetonitrile (50 mm, 0.5 mL) caused remarkable changes
of the proton chemical shifts (Figure S7a,b). Almost all
complexed signals disappeared, sharp signals of uncomplexed
protons H8, H6, and H1 appeared, and the signals of protons
H3 and H4 exhibited upfield shifts. All these observations
suggested that the host–guest interactions were destroyed
completely and the complexation between DB24C8 and DBA
was totally quenched. After 14.0 mL of trifluoroacetic acid
was added, the host–guest complexation was recovered and
the complicated complexed signals were observed again
(Figure S7c).[6b,12] In addition, this reversible decomplexa-
tion–complexation transition could be repeated (Fig-
ure S7d,e).
Also, the host–guest interaction between the DB24C8 and
DBAunits could be reduced by heating, as shown by 1H NMR
1
experiments. The variable-temperature H NMR spectra of
monomer 3 in [D3]acetonitrile (see Figure S8 in the Support-
ing Information) provided direct evidence for the assembly
process from gel to sol state. At a relatively low temperature
1
(268 K), the H NMR signals of monomer 3 almost disap-
peared, suggesting strong intermolecular aggregation. By
gradually raising the temperature, the original weak and
broad signals became well-dispersed and can be easily
identified. These results showed a remarkable temperature-
dependent behavior and suggested that the formation of the
gel was weakened at elevated temperatures and eventually
disrupted,[13] which was consistent with the above gelation test
(Figure 2).
Thus, by adjusting the pH and temperature of the solution,
the gelation process can be manipulated to control a range of
gel properties, such as the gelation time, gel transparency, gel
morphology, and the gel–sol transition.
It is generally known that the secondary ammonium salt
unit can be deprotonated by adding base, thus destroying the
host–guest recognition between DB24C8 and DBA and
making the complex disassemble. Hence, the reversible
gel–sol transition could be realized by changing the pH
value. As shown in Figure 2, after the addition of several
drops of triethylamine, the gel dissociated into a transparent
solution within a short time. Re-formation of the gel from the
sol state was achieved by adding a little excess trifluoroacetic
Xerogels, prepared by freeze-drying the gels of monomer
3 in CH3CN, were examined by SEM, revealing an extended
and interconnected fibrous gel network. The SEM images
showed long fibers and
well-developed
three-
dimensional network struc-
tures of fibers with diame-
ters of 1–2 mm and lengths
of several hundred micro-
meters (Figure 3b). The
formation of fibers is a
typical characteristic for
the entanglement of line-
arly connected macrosized
aggregates. These self-
assembled fibers physically
cross-linked together to
form a fibrous network as
the matrix of the gel.[10a]
This extended network fur-
ther interweaved and tan-
gled with fibers to form a
very dense gel network
Figure 2. Supramolecular gel, its gel–sol transitions triggered by stimuli (temperature and pH), and
supramolecular aggregates (glue-like viscous liquids and transparent films).
Angew. Chem. Int. Ed. 2011, 50, 1905 –1909
ꢀ 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
1907