F. Lin et al. / Tetrahedron 70 (2014) 2251e2256
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above, it was found that the counterions had very little influence
on the stacking of the molecules. These results suggest that aro-
matic stacking should play a crucial role in driving the self-
assembly of these amphiphiles. However, it should be noted that
the structures of aggregates in solution state might not be fully
same as that in the bulk crystals.
inside because a clear contrast between the wall and the inner part
was observed (Fig. 2f), which supported the formation of nano-
tubes. The wall thickness was estimated to be 1.8 nm from the TEM
image. This value was very close to the length (2.08 nm) of T3
measured from its crystal structure, suggesting that the wall of
nanotubes was generated by the monolayered packing of T3.
Compared to T1eT3, the hydrophilic segments of amphiphiles
T4eT6 are more polar. DLS also confirmed that they existed as
aggregates in aqueous media (Fig. S2, SD). Similar to its precursor
T1, T4 also self-assembled into spherical micelles (Fig. 3a). How-
ever, the diameters of the micelles generated from T4 were only
30e40 nm, quite smaller than those from T1, (Fig. 3b). It might be
attributed to the higher charge density of T4, which kept a small
size to reduce electrostatic repulsion. In contrast, compound T5
gave rise to ultra-long nanofibers (Fig. 3c). The solid feature of these
fibers was revealed by TEM (Fig. 3e). As shown in Fig. 3c, the fibers
were quite straight and the lengths of these fibers were estimated
to be >1.0 mm because no ends of the fibers could be observed in
the scope of the SEM image. AFM was further used to characterize
the morphology of the self-assembled structures of T5, which also
revealed the formation of nanofibers (Fig. S3, SD). From the SEM
image of higher resolution, the widths of the fibers were estimated
to be less than 500 nm (Fig. 3d). Since viologens have been widely
used in optoelectronic materials,13 these ultra-long nanofibers
might be further exploited as optoelectronic devices. In contrast to
T4 and T5, T6 gave rise to ill-defined aggregates. This result might
be attributed to its different packing style from the other amphi-
philes and its unmeet hydrophilic/hydrophobic ratio.
Similar to conventional flexible amphiphiles, these wholly-rigid
roderod amphiphilic molecules also possess critical micelle con-
centrations (CMCs). Their CMCs were determined by the specific
conductivity method in water (Fig. S1, SD) and the results provided
in Table 2. For comparison, the CMCs of rodecoil type amphiphiles
T7eT12, which were constructed from the same hydrophilic unit
but flexible alkyl chains of comparable lengths as hydrophobic
segments, were also measured. Specific conductivityeconcentra-
tion plots of solutions of compounds T7eT9 did not show a de-
tectable inflection point, suggesting that their amphiphilic feature
is not obvious. In contrast, compounds T10eT12 exhibited CMCs
and the values are higher than those of T1eT6, indicating the ag-
gregating tendency of the roderod type amphiphiles is higher than
the rodecoil type amphiphiles. This result might be attributed to
the more orientational organization of the stiff roderod structures.
Furthermore, the CMCs of compounds T4eT6 are slightly lower
than their corresponding precursors T1eT3, suggesting T4eT6
exhibit more ‘amphiphilic feature’ due to their dicationic hydro-
philic segment.
Table 2
Critical micelle concentrations of T1eT5 and T10eT12 in water at 25 ꢀC
For comparison, the self-assembling behavior of control com-
pounds T10eT12 in water were also investigated using TEM. It was
found that these compounds all assembled into sphere-like mi-
celles, which was independent on the length of their hydrophobic
tail (Fig. S4, SD). This result clearly demonstrated the difference of
the self-assembling property of the roderod and rodecoil amphi-
philes, even though they share same hydrophilic segments. The
morphology should be dictated by the different hydrophilic/hy-
drophobic ratios of these amphiphiles. Compared to the rodecoil
ones, the roderod amphiphiles were more sensitive to the subtle
change of the hydrophilic/hydrophobic ratio. This feature could be
attributed to the stiffness of the wholly-rigid molecules, which
were hard to alter their conformations during the self-assembling
process. In contrast, the rodecoil structures were semi-rigid and
thus the hydrophilic/hydrophobic ratio might be adjusted by the
change of their conformation.
Compound
CMC/mM
Compound
CMC/mM
Compound
CMC/mM
T1
T2
T3
0.08
0.10
0.081
T4
T5
T6
0.073
0.088
0.076
T10
T11
T12
0.136
0.107
0.092
The self-assembling behavior of T1eT3 in water was then in-
vestigated. Dynamic light scattering (DLS) experiment revealed
that they all aggregated into large species in aqueous media (Fig. 2a
and Fig. S2, SD). The average hydrodynamic diameter (Dh) of the
aggregates formed by T1 in the aqueous solution was estimated to
be 190 nm (Fig. 2a). Transmission electron microscopy (TEM)
revealed that T1 gave rise to spherical micelles and the diameters of
the micelles were estimated from the TEM image to be in a range of
100e200 nm (Fig. 2a), which is consistent with the value obtained
from DLS. Under the similar conditions, T2 self-assembled into one-
dimensional (1D) fibrous morphology with the diameter being ca.
2 microns (ca. 350 nm at lower concentration, see the TEM below),
as demonstrated by scanning electron microscopy (SEM) (Fig. 2c).
The SEM image also clearly revealed that the microfibers were solid
inside from the visible cylindrical section of the end of one fiber
(Fig. 2c, inset). The fibrous morphology was also revealed by atomic
force microscopy (AFM) image (Fig. S3, SD). This solid feature was
further evidenced by the TEM image, which displayed no contrast
between the inner part and the peripheral part (Fig. 2d). It was
found that T3 also self-assembled into 1D structures, with their
lengths being several hundred microns and widths being hundreds
nanometers (Fig. 2e). However, different from those fabricated from
T2, TEM revealed that the fibers assembled from T3 were hollow
3. Conclusion
In summary, a series of wholly-rigid roderod amphiphiles have
been constructed and their self-assembling properties have been
investigated. Generally these new compounds exhibit the typical
amphiphilic feature possessed by conventional flexible amphi-
philes and thus can self-assemble into diverse well-defined archi-
tectures of different morphologies, depending on the hydrophilic/
hydrophobic fraction ratio of the molecule. However, the new rigid
amphiphiles also exhibit their own feature by displaying a higher
assembly tendency and a preferred tendency of forming 1D struc-
tures with high stiffness. The behavior exhibited by these novel
amphiphiles is different from the previously reported roderod
block copolymers, which prefer to self-assemble into low-curvature
vesicular or lamellar structures and the morphologies assembled
from them are independent on the specific chemical structure and
composition of the copolymers.14 We believe systematic studies on
more roderod amphiphilic structures will uncover more intriguing
properties of this new family member of amphiphiles. Further
study is pointing to the roderod bolaamphiphiles and gemini
amphiphiles.