To study the molecular organization that leads to the fibrillar
structure observed in the SEM images, X-ray diffraction (XRD)
analyses were performed on films of PAM 1 obtained from a
cyclohexane gel (1.0% w/v) and compared to a film made from
PAM 1 in a THF solution for which no gelation was observed
at this concentration. The diffractogram (see Figure S2 in the
ESI†) of the dried gel showed a sharp intense peak at 2q =
2.5, which corresponds to 3.52 nm. The data extracted from
the diffractogram are not clear enough to confirm any particular
arrangements within the gel. Nonetheless, based on other reports
on PAM assemblies,6,15 it can be hypothesized that the macrocycles
stacked on top of each other to form columnar assemblies with an
intercolumnar distance of ca. 4 nm, which is in good agreement
with the calculated width of PAM 1. The columnar arrangement
is also in good agreement with the fibrillar structure observed by
SEM. Interestingly, no feature except a broad band centered at
2q ª 24, which is representative of an amorphous material, was
observed when a film of PAM 1 was formed from a THF solution.
This is indicative of the importance of the gelification process for
obtaining a well-ordered array of macrocycles.
In summary, we have prepared a phenylacetylene macrocycle
that shows excellent gelation properties in many organic solvents.
Characterization reveals the formation of nanofibrils that consist
of stacks of macrocycles owing to intermolecular hydrogen bond-
ing as showed by the FTIR analysis as a function of temperature.
The interactions strengthen the supramolecular organization and
open the way to the utilization of PAMs as robust building blocks
for the preparation of nanoscale functional materials. PAM 1
is now being studied as a potential precursor in topochemical
polymerization to build covalently linked organic nanotubes.
Fig. 2 SEM images of the organogel from PAM 1 (a) in toluene, scale
bar = 1 mm, and (b) in cyclohexane, scale bar = 50 mm.
PAM 1 in toluene (1.0 w/v%) is made of microns-long 1D wirelike
fibers with diameters of few tens to few hundreds of nanometres.
These nanofibers assembled into much larger bundles, which is
indicative of strong interfiber interactions. Interestingly, the size
of the fiber obtained after the gelification process is dependant
on the nature of the solvent. As shown in Fig. 2b, much larger
fibers than those obtained from toluene gel (Fig. 2a) are observed
when cyclohexane is used at the same gel concentration (1.0%
w/v). In this particular case, microns-wide fibers are obtained, and
although the internal structure of the fibers is difficult to observe,
one can argue that the fibers are made of aligned smaller fibers.
At this point, the parameters that lead to different assembly from
one solvent to another are not well understood and a systematic
study of fiber width–solvent dependence is being conducted.
To assess whether or not the amide groups allow the formation
of intermolecular H-bonding, Fourier transform infrared (FTIR)
spectra were recorded on a gel of PAM 1 at different temperatures.
The results are shown in Fig. 3. For this study, the gel was prepared
in decalin because a high boiling point solvent was needed to avoid
solvent loss during the experiment.
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Fig. 3 FTIR of a 1.0 w/v% organogel of PAM 1 in decalin as a function
of the temperature.
At 20 ◦C, the associate Amide I and Amide II bands were
observed at 1640 and 1542 cm-1, respectively. Upon heating, the
bands gradually disappeared, as the H-bonds broke, and a new
band at 1685 cm-1 attributed to the free Amide I band appeared.
Unfortunately, the band associated with the free Amide II band
was hidden by the decalin peak in the 1400–1520 cm-1 region.
These spectral changes strongly support the formation of inter-
molecular H-bonding that contributed to the gelation ability of
PAM 1 in addition to possible p–p and van der Waals interactions.
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4442 | Org. Biomol. Chem., 2011, 9, 4440–4443
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