Macromolecules
Article
methanol, ethanol, and DCM. The good solubility can be
assigned to two reasons: (1) the main-chain-type structure of the
poly(arylene−imidazolium) and (2) the large steric hindrance
of the imidazolium cations. These two factors make the ionic
groups on the polymer chain have a strong mutual repulsion
effect, which reduces the entanglement of the polymer chain and
increases the solubility. However, poly-PhIM [OH] was
insoluble in alkaline solution even at high temperatures. This
behavior was also exhibited by the polyarylimidazole poly-
electrolyte reported by Fan et al.22 The introduction of
hydrophobic biphenyl segments caused the solubility of poly-
PhIM-b-biPh [OH] and poly-PhIM-co-biPh [OH] to be
somewhat different from that of poly-PhIM [OH]. In pure
water, these two copolymers cannot be dissolved even at 100 °C.
Additionally, their solubility in alcohol was reduced to a certain
extent.
The role of the biphenyl segment was also reflected by the
improvement in mechanical properties (Table 1). The tensile
strength of homopolymer poly-PhIM [OH] was only 1.43 MPa.
Differently, the tensile strength of two copolymers increased 10-
fold owing to the introduction of the biphenyl segment. This can
be assigned to the π−π interaction of the aromatic ring in the
biphenyl segment, which effectively enhanced the chain
entanglement of the polymer. Moreover, the block-like polymer
has a higher elongation at break and Young’s modulus, while the
random copolymer has higher tensile strength. This provided a
new idea for adjusting the mechanical properties of ionomers by
controlling the order of feeding into the reaction system.
Water Uptake, Swelling Ratio, Conductivity, and
Micromorphology. The water uptake and swelling ratio of
poly-PhIM [OH], poly-PhIM-b-biPh [OH], and poly-PhIM-co-
biPh [OH] are summarized in Figure 5a. Compared with poly-
PhIM [OH], the two copolymers showed a much lower water
uptake and swelling ratio. This is because the introduction of
hydrophobic biphenyl fragments reduces the IEC of the
copolymer membranes, making the membranes insoluble in
water and having lower water uptake. In addition, the block-like
copolymer poly-PhIM-b-biPh [OH] simultaneously showed a
higher water uptake and swelling ratio than the random polymer
poly-PhIM-co-biPh [OH]. A comparison of the photographs of
the three samples under dry and wet conditions is shown in
Figure 5b; at 80 °C, in a hydrated state, poly-PhIM [OH] is
basically dissolved, the block-like copolymer swells very
obviously and becomes opaque, and the random copolymer
does not change significantly. This can be attributed to
hydrophilic and hydrophobic segments being randomly
distributed in the random copolymers, thus interrupting the
continuous aggregation of the hydrophilic regions, effectively
limiting the water absorption capacity.
absorption diluting the OH− concentration. The lower water
uptake of the random copolymer at high temperatures endowed
it with a higher OH− concentration, effectively improving its
conductivity. In short, in addition to the chemical structure of
the monomer, this study showed that the length and sequence of
the control block-like polymers are directly related to the ion
transport opening new avenues for future studies on the
structure−activity relationship of AEMs.
The micromorphology of poly-PhIM [OH], poly-PhIM-b-
biPh [OH], and poly-PhIM-co-biPh [OH] was first investigated
in their dry state via small-angle X-ray spectroscopy (SAXS). As
shown in Figure S13, no obvious ionomer peak was detected in
the range q = 0.1−1.9 nm−1, which may be due to the fact that
the main-chain-type ionomer structure makes the difference in
electron cloud density between hydrophilic and hydrophobic
regions insignificant. Then, to further study their micro-
morphology, AFM and TEM measurements were carried out.
In Figure 6a−f, evident light and dark regions were observed in
the AFM phase diagrams of the three polymers at the scales of
1.0 μm × 1.0 μm and 500 nm × 500 nm, suggesting the
difference between the hydrophilicity and hydrophobicity
(softness and hardness) on the surface of the polymers, which
may be a manifestation of phase separation. The TEM images in
Figure 6g−i show the microstructures of poly-PhIM [OH],
poly-PhIM-b-biPh [OH], and poly-PhIM-co-biPh [OH] at the
nanoscale, respectively. The test membrane samples were
stained with H2PtCl6 in advance to achieve an exchange of
OH− to PtCl62−. The dark regions reflect the ionic hydrophilic
domains and the light regions show the hydrophobic domains
(alkyl chain and biphenyl segments), which suggest the
formation of well-defined phase-separated structures in the
membranes. Although they are main-chain-type polymers, the
hydrophilicity and hydrophobicity of the long alkyl substitutes at
the position N1/N3 of the imidazolium ring are quite different
from that of the ion center, so the phase separation structure
described above exists. Moreover, the size and shape of the ion
clusters of the three polymers are different from each other,
which may be due to the difference in the content of the
imidazolium cation and the different distributions of the
imidazolium segments, so that different water absorption
properties and conductivities are finally obtained.
Thermal Stability and Alkaline Stability. The thermal
stability of poly-PhIM [OH], poly-PhIM-b-biPh [OH], and
poly-PhIM-co-biPh [OH] was studied by thermogravimetric
analysis (TGA) and differential thermogravimetry (DTG)
(Figure S14). According to the TGA curve, below 200 °C, a
small amount of weight loss is associated with the evaporation of
residual solvent and water in the membranes. Due to the
excellent thermal stability of imidazolium cations, all three
samples began to decompose at very high temperatures (>350
°C). Based on DTG data, the temperature point of
weightlessness can be judged more accurately. The decom-
position temperatures of poly-PhIM [OH], poly-PhIM-b-biPh
[OH], and poly-PhIM-co-biPh [OH] are 434.9, 429.9, and 435.4
°C, respectively. Here, poly-PhIM [OH] and poly-PhIM-co-
biPh [OH] undergo similar thermal degradation processes.
Differently, the thermal decomposition of poly-PhIM-b-biPh
[OH] includes two stages. In addition to the first stage, there is
another decomposition process at 535.6 °C, which can be
attributed to the decomposition of the biphenyl segments within
the block-like copolymer. These findings indicate that the
difference in the structure of the chain segments will be reflected
in the thermal decomposition process of the polymers.
Ionic conductivity is one of the most important factors in
determining fuel cell performance.35,36 The hydroxide con-
ductivity of the three polymers is summarized in Figure 5c.
Although their IEC values are not high, these poly (arylene−
imidazolium)-based AEMs still have excellent conductivity of up
to 60−70 mS cm−1 at 80 °C under fully hydrated conditions
(Table 1). Additionally, the block-like and random copolymer
showed evidently different OH− conduction behavior. Between
30 and 60 °C, as for the block-like polymer, its conductivity
increased rapidly with the increase in temperature. In contrast,
the conductivity increase rate for the random copolymer was
significantly lower than that of the block-like copolymer. Above
60 °C, the conductivity increase rate for the block-like polymer
slowed down, which might be attributed to the excessive water
2209
Macromolecules 2021, 54, 2202−2212