point of the solvent and slowly cooled down to room
temperature. Compound 1 showed good gelation ability
in all the aromatic solvents tested (see Table S1 in the
Supporting Information). In fact, aromatic solvents al-
lowed gel formation at low concentration in o-DCB (2.5
mg/mL) and toluene (3.0 mg/mL). Depending on the
solvent used, the gel obtained is translucid, semitranslucid,
or opaque (Figure S1 in the Supporting Information). This
behavior can be attributed to different solublities of com-
pound 1 in aromatic solvents, leading to gels having
various levels of crystallinity. In all the aromatic solvents
tested, repeating the heating/cooling process alwayslead to
similar gels. In nonaromatic solvents, many states are
obtained including a viscous solution, solution, or simply
suspension of insoluble material. In contrast to compound
1, compound 2 was found to be insoluble at room tem-
perature in all the solvents tested. Even after heating a
suspension of compound 2 in different solvents, precipita-
tion rather than gelification occurred. This difference
between both compounds is indicative of the importance
of the hydroxy-ethoxy chain attached to compound 1 for
the assembly process. In addition to increasing the solubi-
lity, they are expected to participate in intermolecular
H-bonding (OH..OH) that supports the formation of a gel.
In order to investigate the crystallization temperature of
solvents within the gel and the thermal stability of the gel,
two gel samples were prepared with either toluene or o-
DCB as solvent at a 10 mg/mL concentration and sub-
jected to differential scanning calorimetry (DSC). In o-
DCB, the DSC analysis was carried at temperatures ran-
ging from 298 to 223 K. A very sharp exotherm attribuable
to the crystallization of supercooled solvent was observed
at 232 K (ΔH = 11.0 kJ/mol) (see Figure S2 in the
Supporting Information). This is approximatively 24 K
below the freezing point of free o-DCB (256 K). By heating
the gel from 223 to 298 K, an endotherm was observed at
257.6 K (ΔH = -11.1 kJ/mol), which corresponds to the
melting point of free o-DCB. A similar phenomenon was
observed for a toluene-based gel.
1 is made of micrometers-long 1-D wirelike fibers with
diameters of a few tens of nanometers. Interestingly, most
of the fibers assembled into well-ordered micrometers-
wide bundles, indicating strong interfiber interactions.12
After irradiation for 24 h, the fibrillar structure was
completely lost as a possible consequence of the destruc-
tion of the H-bonding network (Figure 2b). This result is in
agreement with the loss of the gel state observed upon gel
irradiation.
In order to study the intermolecular interactions and
distances within the supramolecular assembly, a gel of
compound 1 (toluene, 10 mg/mL) was deposited onto a
glass slide, slowly dried at room temperature, and sub-
jected to XRD analysis. A recording of XRD spectra was
taken between angles of 2θ = 1° and 15° (see Figure S3 in
the Supporting Information). The diffraction pattern is
˚
characterized by three peaks at 22.9, 11.4, and 7.5 A, which
correspond to a 1:1/2:1/3 ratio. This peak pattern is
indicative of the presence of a layered structure with an
interlayer distance of 2.3 nm.13 To draw a comparison, a
sample of compound 1 was dissolved in MeOH and cast
onto a glass slide substrate. XRD analysis after drying did
not show any crystallographic peaks, thus confirming the
lack of arrangement in the solid state (see Supporting
Information).
Photopolymerization was achieved on a 10 mg/mL
toluene gel of 1 by irradiation at 254 nm with a 120 W
UV lamp at a distance of 2 cm for 6 h. The blue state
generally associated with the highly extended π-delocaliza-
tion along the polydiacetylene backbone14 was never
reached in the gel form. Also, after a dark orange form
was obtained, a loss of the gel state and the appearance of a
red, translucent solution after 6 h of irradiation were
observed (Figure 3). This phenomenon observed by
To gain a better understanding of the nanoscale mor-
phology of the organogel, a small portion of it was slowly
dried under ambient conditions onto a metallic substrate
and subjected to scanning electron microscopy (SEM)
analysis. Asshown inFigure2, theorganogel ofcompound
Figure 3. (a) Compound 1 in the gel form (10 mg/mL in toluene)
at room temperature; (b) the same gel after irradiation at 254 nm
for 4 h; and (c) the gel evaporated on a glass slide and irradiated
for 24 h at 254 nm.
Moreau et al. during the photopolymerization process of
alkyl-substituted butadiyne derivatives could be attributed
to a significant conformational change of the aryl groups
within the gel, thus disturbing the hydrogen bond network.2g
(12) Zhang, P.; Wang, H.; Liu, H.; Li, M. Langmuir 2010, 26, 10183–
10190.
(13) (a) Abdallah, D. J.; Sirchio, S. A.; Weiss, R. G. Langmuir 2000,
16, 7558–7561. (b) Hanabusa, K.; Matsumoto, M.; Kimura, M.;
Kakehi, A.; Shirai, H. J. Colloid Interface Sci. 2000, 224, 231–244.
Figure 2. SEM images of organogel from compound 1 in toluene
(10 mg/mL) before (a) and after (b) irradiation for 24 h at 254
nm. The scale bars are 1 and 0.5 μm for (a) and (b), respectively.
€
(14) Wenz, G.; Muller, M. A.; Schmidt, M.; Wegner, G. Macro-
molecules 1984, 17, 837–850.
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Org. Lett., Vol. 13, No. 6, 2011