Open Access Article
Richard Webera,
Malte Klingenhofb,
Oleksandr Dolynchuk
c,
Luis Hagner
de,
Lukas Metzler
de,
Susanne Koch
de,
Mario Zersonag,
Robert Magerle
ag,
Peter Strasser
b,
Severin Vierrath
de and
Michael Sommer
*af
aInstitute of Chemistry, Chemnitz University of Technology, Straße der Nationen 62, 09111 Chemnitz, Germany. E-mail: michael.sommer@chemie.tu-chemnitz.de
bDepartment of Chemistry, Technical University Berlin, Straße des 17. Juni 124, 10623 Berlin, Germany
cInstitute of Physics, Martin Luther University Halle-Wittenberg, Van-Danckelmann-Platz 3, 06120 Halle, Germany
dElectrochemical Energy Systems, IMTEK-Department of Microsystems Engineering, University of Freiburg, Georges-Koehler-Allee 103, 79110 Freiburg, Germany
eHahn-Schickard, Georges-Koehler-Allee 103, 79110 Freiburg, Germany
fResearch Center for Materials, Architectures and Integration of Nanomembranes (MAIN), Chemnitz University of Technology, Rosenbergstr. 6, 09126 Chemnitz, Germany
gInstitute of Physics, Chemnitz University of Technology, Reichenhainer Straße 70, 09126 Chemnitz, Germany
First published on 18th May 2026
The development of membranes for anion exchange membrane water electrolysis (AEMWE) has recently been extremely fruitful, but less effort has been devoted to specific tailoring of polymeric binders to enhance catalyst utilization and electrical conductivity within the catalyst layer. Herein we report a simple one-pot synthesis of block copolymers (BCP) for application as anode binders in AEMWE. The BCPs contain hydrophilic poly(biphenyl piperidinium) and hydrophobic blocks based on meta-terphenyl and 2,2,2-trifluoroacetophenone of varying fractions. The synthetic approach provides facile access to ionomers with largely varied ion exchange capacities (IECs) between 0.94 and 2.68 meq. g−1, giving rise to binders with extremely low swelling yet efficient hydroxide transport. The least hydrophilic BCP with ∼25 wt-% hydrophilic fraction and an IEC of 0.94 meq. g−1 exhibits a high hydroxide conductivity of σOH = 174 mS cm−1 at 80 °C at a low water uptake of 13% at 80 °C, and almost temperature-independent swelling. The low water uptake enables increased catalyst utilization in nickel-iron layered double-hydroxide-based anodes, which, in combination with the high hydroxide conductivity, results in an improved AEMWE performance. AEMWE single cells exhibit current densities of 3800 mA cm−2 at 2 V, not achieved neither by using statistical copolymer analogs nor commercial-type binders.
The role of the binder to help form an optimal MEA morphology is also key for ideal catalyst utilization within the so-called triple-phase-boundary.5,32,33 Here, a low water uptake (WU) and a low swelling is beneficial to maintain contact of catalyst particles and hence improve electrical conductivity within the catalyst layer.34 A low swelling has also been reported to improve the stability of AEM electrolyzers.20 Similarly, for quaternized polystyrene ionomers a high IEC of the binder is of disadvantage for long-term operation of AEMWE, since catalyst particles may detach from the MEA.11 Somewhat in contrast, we previously found that within a series of poly(terphenyl piperidinium)s used as binders, an increasing WU led to higher hydroxide conductivities, catalyst utilization and improved AEMWE single cell performance.35 This emphasizes the necessity for a more profound understanding of the interplay of the diverse functions of the ionomer binder that contribute to AEMWE performance and stability.
Strategies to tune, control and limit swelling of AEMWE materials are manifold, and have mostly been reported in the context of membranes rather than binders. These include, but are not limited to, reinforcements,36 fluorination,37 branching,38 multi-cationic side-chains39 or crosslinking.40 Similarly, by virtue of phase-separation of block copolymers (BCP) or segmented architectures in general, hydrophilic, ion-containing segments may segregate into domains of high charge density to optimize ion transport. Eventually, the remaining compartments may be tailored to meet further criteria such as mechanical strength or gas permeation. BCPs with cationic groups can be prepared by e.g. ring-opening metathesis polymerization,41 radical polymerization,42 polyinsertion10,43 or polyhydroxyalkylation.42,44 To name examples, BCPs prepared by atom-transfer radical polymerization showed a WU of 123% at 80 °C and a hydroxide conductivity (σOH,80) of 81 mS cm−1 at 80 °C.42 Pentablock polynorbornenes made via vinyl addition polymerization reached a WU of 85% at 25 °C and a σOH,80 of 100 mS cm−1 at 80 °C.43 Using polyhydroxyalkylation, poly(biphenyl alkylene) block copolymers with ammonium side-chains delivered a σOH of 162 mS cm−1 at 108% WU and 80 °C, and were deployed as membranes and binders simultaneously.44 However, dedicated studies aiming to vary and understand binder properties are much less prevalent compared to the large body of literature available on membranes. Considering the key role of the binder for optimizing morphology of the triple-phase-boundary, BCPs appear highly promising.
Herein, we report a simple one-pot synthesis of block copolymers via polyhydroxyalkylation for application as anode binder ionomers in AEMWE and compared their performance with statistical copolymer analogs of identical composition. Varying the ratio between the hydrophilic poly(biphenyl piperidinium) (PBP) block and the hydrophobic block based on meta-terphenyl and 2,2,2-trifluoroacetophenone yields BCPs with largely varied ion exchange capacity (IEC), and thus swelling properties. The hydrolytic stability of the BCP binders increased with increasing IEC as a result of the increased nucleophilicity of the hydroxide anion under low hydration conditions. The BCP with ∼25 wt-% hydrophilic fraction exhibited a high hydroxide conductivity (σOH = 174 mS cm−1) at very low IEC (0.94 meq. g−1) and thus low hydration (WU = 13%), leading to superb binder capability when used as binder in nickel-iron layered double-hydroxide (NiFe-LDH)- based anodes. A binder pre-screening via rotating disk electrode (RDE) experiments correlated well with AEMWE single cell testing, revealing that the low IEC binder outperforms all other BCPs, statistical as well as commercial-type poly(arylene piperidinium) analogs. Current densities of 3800 mA cm−2 at 2 V were obtained in AEMWE single cell tests with the best BCP, which is approx. 1000 mA cm−2 higher compared to commercial PiperION-A. This improvement in performance is explained by the synergistic effect of the low IEC enabling enhanced catalyst utilization as a result of a better electrical conductivity within the catalyst layer, combined with a simultaneously improved hydroxide conductivity.
The number and weight average molar weights and dispersities determined via SEC are compiled in Table 1. All final copolymers were purified via Soxhlet extraction with methanol and subsequently acetone to remove oligomers and yield comparable molar masses. Fig. S3 monitors the success of Soxhlet extraction. Fig. 1 shows the SEC curves of the three individually prepared hydrophilic starting blocks of almost identical molar masses (Mn,SEC = 4.1–4.5 kg mol−1) together with the corresponding final BCP products. All chromatograms of the BCPs were shifted towards lower elution volumes with vanishing intensity in the region of the starting block, which confirms the success of the synthetic strategy. The 1H NMR spectra of the BCPs further proved the presence of both hydrophilic and hydrophobic segments, confirming a successful linkage of hydrophilic and hydrophobic blocks (Figures S4–5). The IECs and compositions were determined via 1H NMR spectroscopy as well as from titration (Table 1).
| Polymer | Mn/kg mol−1 | Mw/kg mol−1 | Ð | wt% hydrophilic | IECth (Cl−)/meq. g−1 | IECth (OH−)/meq. g−1 | IECtitr (Cl−)/meq. g−1 |
|---|---|---|---|---|---|---|---|
| BCP_79 | 24 | 71 | 3.0 | 79 | 2.68 | 2.82 | 2.34 |
| stat_73 | 57 | 177 | 3.1 | 73 | 2.48 | 2.61 | 2.50 |
| BCP_55 | 37 | 88 | 2.4 | 55 | 1.90 | 1.97 | 1.85 |
| stat_46 | 30 | 72 | 2.4 | 46 | 1.59 | 1.64 | 1.54 |
| BCP_26 | 39 | 98 | 2.5 | 26 | 0.92 | 0.94 | 0.71 |
| stat_22 | 34 | 57 | 1.7 | 22 | 0.77 | 0.79 | 0.97 |
To study the bulk morphology of the prepared ionomers, small-angle (SAXS) and wide-angle X-ray scattering (WAXS) experiments were performed on dry (with iodide as counter ion) as well as on wet polymers (hydroxide form) (Fig. 2). In the dry state, BCP_26 and BCP_55, but not BCP_74, showed a very broad and weak SAXS scattering intensity in the 0.03 Å−1 < q < 0.2 Å−1 region. This corresponds to density variations on length scales of 3 to 20 nm without long-range order (Fig. 2a). The broad distribution of SAXS intensity that is also clearly seen in a double-log plot is a clear difference compared to the statistical polymers that did not show any scattering intensity in the same region (Fig. S6). The WAXS pattern of BCP_26 featured three additional peaks (red lines in Fig. 2a) that resemble those of the corresponding hydrophobic homopolymer (see Fig. S7). These WAXS peaks were not visible in the patterns of the less hydrophobic BCP_55 and BCP_79 and indicated the ability of the hydrophobic block to order on a length scale of ∼1 nm. The WAXS pattern of the dry stat_22, however, showed these same peaks, albeit with lower intensity. This indicates that the distribution of monomers in the statistical copolymer is not entirely random, but segmented to some extent. To underline this hypothesis further, we investigated the development of molecular weight of the four possible homopolymers with time. For the combination of BP and Pip, the increase in molecular weight was strongest due to the larger electrophilicity of N-pip compared to TFAp and the higher reactivity of BP compared to mTP, corroborating the idea of segmentation (Fig. S8). This would allow segments similar to the hydrophilic starting blocks used for BCP synthesis to form.
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| Fig. 2 SAXS and WAXS patterns of (a) dry polymers in iodide form and (b) polymers after water uptake (hydroxide form). The curves are shifted vertically for clarity. | ||
The SAXS curves of the wet block copolymers showed distinct changes upon water uptake (Fig. 2b). While BCP_55 and BCP_79 showed an increase in scattering intensity with increasing fraction of the hydrophilic block, the broad and weak peaks of the dry BCP_26 vanished. For BCP_79, a d-spacing of 4.6 nm was observed. For BCP_55, two SAXS peaks corresponding to d-spacings of 8.8 and 3 nm were found, i.e. the long period of BCP_55 shifted to lower q values compared to the dry sample. Such humidity-dependent swelling and corresponding shifting of SAXS “ionomer” peaks to lower q values is well known for proton conducting membranes and indicates clustering of hydrophilic parts of the chain with water.48,49
The vanishing SAXS peak of the wet BCP_26 is not surprising considering that the rather irregular, poorly ordered structure of the dry sample may become even less regular upon swelling. The fact that the three WAXS peaks of wet BCP_26 were retained to some extent indicates that the order of the hydrophobic part is preserved upon swelling (note that the different overall shapes of the WAXS patterns of the dry and wet samples are caused by the different measurement conditions, the use of a sealed glass capillary, and the presence of water).
Compared to the BCPs, the SAXS curves of the hydrated membranes made from the statistical copolymers were qualitatively similar, albeit showing less defined peaks. Also here, the scattering intensity increased with increasing water content. For stat_46 and stat_74 two broad peaks were observed corresponding to the characteristic distances of 4.7 and 4.3 nm, respectively.
Compared to classical BCP self-assembly,50 the herein made BCP samples show poor order on the 3 to 20 nm length scale. This is not surprising considering their large dispersities (see Table 1) as well as the fact that with decreasing hydrophobic fraction, the probability for the formation of multiblock architectures increases. Furthermore, it is possible that monomer scrambling occurs during the synthesis of the second block as a result of transalkylation,51 i.e. as soon as the mixture of mTP and TFAp is added. Although the molar mass of the hydrophilic block was shown to be stable in the absence of the second portion of hydrophobic monomers (c.f. Fig. S1), such fragmentation process would decrease the initially formed hydrophilic block length leading to a reduced tendency for phase separation. To this end, a model experiment was conducted in which an excess of BP was added to a freshly grown hydrophilic block, resulting in a decrease of Mn,SEC from 22 to 17 kg mol−1 within 2 h (Fig. S9). Thus, monomer scrambling seems possible upon addition of mTP and TFAp under acidic conditions. However, to what extent such process has been present during the synthesis of BCP_26 cannot be probed directly, and so the correlation of redistributed hydrophilic and hydrophobic monomers in the chain with the absence of a SAXS peak remains to be proven. If present, the resulting segment distribution is governed by the mechanism of the polyhydroxylation reaction, and the morphologies of the final BCP products would certainly be influenced.
Overall, the processes of segmentation of statistical copolymers and possibly fragmentation of the first block during the synthesis of the second cause a rather complex chain sequence and render full control over chain architecture challenging. While clear differences in the phase behavior of the BCP and stat samples remain, we note that these two processes could finally lead to more similar chain sequences than anticipated. To further characterize the nanomorphology of the membranes, thin BCP films were imaged with atomic force microscopy (AFM) in the dry state (Fig. 3a–c). BCP_26 exhibited a terrace-like surface topography, with a step height of approximately 2–2.5 nm between the terraces. In contrast, BCP_55 and BCP_79 showed a smooth surface with fine granular domains. The broad SAXS scattering intensity of dry BCP_55 and BCP_79 indicated density variations on length scales of 3 to 20 nm without long-range order (Fig. 2a). This is consistent with the fine-grained morphology of the thin film surface of these samples. To obtain information on the phase separation of two homopolymers in general, a µm thick blend film was prepared (25 wt-% hydrophilic PBP and 75 wt-% poly(meta-terphenyl 2,2,2-trifluoroacetophenone), PmTPTFAp). This film showed large, spherical domains of PmTPTFAp of up to 200 µm embedded in a matrix of PBP (Fig. 3d). This is a clear indication for a rather strong tendency of the two homopolymers to phase separate. Visually, the homopolymer blend film appeared turbid, while the BCP films were fully transparent. This is consistent with the domain sizes observed using SAXS, AFM and optical microscopy (Fig. 3e and f).
The water uptake (WU) and swelling behavior of the BCPs was investigated and compared to the statistical copolymers. Fig. 4 shows the WU, hydration numbers, through-plane swelling ratio and areal swelling, as a function of temperature. The WU and hydration numbers (λ) were governed by the fraction of the hydrophilic block. WU further increased with temperature for all samples, with an increase that was stronger with higher IEC (Fig. 4a and b).
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| Fig. 4 Water uptake WU (a), hydration number λ (b), through-plane (c) and areal swelling ratio (d) of the block versus statistical copolymer. | ||
The swelling ratio (SR) for BCP_26 and stat_22 remained at a similarly low level and was mostly independent of temperature (Fig. 4c and d). Furthermore, the higher the IEC, the stronger WU and λ were increasing. The BCPs span a broad range of WU values, with BCP_79 and BCP_26 exhibiting the highest and lowest water uptake of 92% and 13% at 80 °C, respectively. The statistical copolymers behaved similarly, with notable differences in WU and λ resulting from slightly varied composition compared to the BCPs as well as from the assumed similar monomer distribution. The temperature-independent swelling behavior of BCP_26 and stat_22 renders them ideal for binder applications since minimal tension is expected in the catalyst layer upon changing conditions. We anticipate the low WU and the temperature-independent swelling of BCP_26 to stem from both the small weight fraction of the hydrophilic block as well as from the ability of the hydrophobic block to retain order also in the hydrated state (see WAXS pattern in Fig. 2). Fig. 5a and b depict temperature-dependent (Fig. 5a) and hydration number-dependent (Fig. 5b) hydroxide conductivities. In all cases, the conductivities increased with temperature in a similar manner. Due to the temperature-dependent conductivity but temperature-independent water uptake of BCP_26, the conductivity versus hydration number plot was rather steep (Fig. 5b), such that a small change in hydration caused a large change in hydroxide conductivity. The activation energies (Ea) of hydroxide transport are given in Table S1. With increasing IEC, the Ea of the statistical copolymers decreases. The same is observed in case of the BCPs except for BCP_26, which shows a significantly lower Ea than stat_22. This supports the observation of better-connected ion transport channels. BCP_79 and stat_73 reached similarly high hydroxide conductivities at 80 °C but required substantially larger amounts of water and accordingly swelled much stronger. The BCP and stat samples with balanced hydrophilic/hydrophobic fractions showed the lowest values of hydroxide conductivity (76 mS cm−1). The highest hydroxide conductivity of 174 mS cm−1 was measured for BCP_26 at 80 °C. This is remarkable considering that this sample featured the lowest IEC (0.94) and the lowest WU (13%) of all BCP samples, suggesting potential use in membrane applications also. When normalizing σ (OH−) by IEC (Figure S10), BCP_26 showed again the highest ion conductivity, confirming the benefit of the block copolymer architecture in terms of phase separation and ionic transport.
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| Fig. 5 Hydroxide conductivity depending on temperature (a) and hydration number (b) of the investigated copolymers. | ||
It is also remarkable that BCP_26 exhibits similar SAXS (Fig. 2a and c) and temperature-dependent WU behavior (Fig. 4a) compared to the statistical sample stat_22, but a significantly higher hydroxide conductivity at lower hydration values. While the presence of a SAXS peaks is often considered a necessary prerequisite for a material to exhibit a beneficial morphology for ion transport,42,52 the different conductivity behavior of BCP_26 and stat_22 may reflect subtle morphological differences not captured by the herein used scattering techniques.
The hydrolytic stability of all copolymers was evaluated in membrane form in 2 M NaOH at 90 °C (Fig. S11–S14), and followed by 1H NMR spectroscopic analysis.24 An increasing IEC correlated with an increasing hydrolytic stability of the piperidinium cation, along with the known degradation pathways of quaternary ammonium groups in alkaline media. It is interesting to note that a lower IEC strongly reduced stability, as a result of the higher nucleophilicity of the hydroxide anion under low hydration conditions.53 For the future use of low IEC binders, hydrolytically more stable cations other than dimethyl piperidinium should be incorporated.54–59
To evaluate the potential of the BCPs to act as binders in catalyst anode layers for the oxygen evolution reaction (OER), rotating disk electrode (RDE) experiments were conducted (Fig. 6). Disk electrodes were prepared from all BCP samples and referenced against the three analogous statistical copolymers as well as further statistical, literature-known copolymers consisting of mTP, para-terphenyl (pTP), Pip and TFAp, hereafter referred to as M0 (self-made PiperION-A) and M100 (analog with 100% mTP instead of pTP). These two polymers have been previously studied as binders, with M100 yielding significantly enhanced performance under similar conditions.35 As a non-precious metal catalyst, nickel iron layered double hydroxides (NiFe-LDH) was used.35 RDE measurements were conducted in 0.1 M KOH solution at room temperature and a rotation rate of 1600 rpm. Fig. 6a and b clearly show that the ionomers with the lowest hydrophilicity exhibited the best OER performance. An increasing hydrophilicity decreased the OER performance for all copolymers. However, not only BCP_26 showed high OER activity. Also, stat_22 as binder gave an OER activity of almost the same level. The fact that stat_22 exhibited a substantially lower hydroxide conductivity indicates this was not the prime factor determining RDE performance. This assumption is further confirmed by the performance of BCP_55 and BCP_79, which had reversed trends of conductivity and current density. To further evaluate the stability of the disk electrodes, the RDE performance was also studied after 25 cyclic voltammograms (Fig. 6c–e). A significant loss of performance was only observed for all copolymers with low initial RDE performance. This decrease is explained by microbubble formation where the catalytically active sites are blocked by oxygen due to limited escape of the product gas.60
The enhancement of reaction kinetics and cycling stability seems to be strongly related to the IEC and the WU of the ionomer binder. This is also visible from the strong oxidation peak around 1.45 V when using BCP_26 and BCP_55 as binders (Fig. 6a). While the large WU of BCP_74 likely separates the catalyst particles, BCP_26 and stat_22 binders allow for sufficient electrical contact, causing a more pronounced oxidizing peak at 1.45 V and hence higher current densities. Thus, we find a strong correlation of RDE performance with IEC, WU and swelling, but not hydroxide conductivity, such that lowering WU increases current density. We rationalize this result by assuming that low IEC binders that are less hydrated improve contact of catalyst particles and electrical conductivity of the catalyst layer, ultimately leading to enhanced catalyst utilization. Similar effects have been reported for Pt/carbon model electrodes with Nafion as binder, for which an increasing relative humidity led to increased electrical resistance.61
In our case, humidity is not varied within one experiment but the hydration level increases from BCP_26 to BCP_55 to BCP_79. Interestingly, stat_22 has an even lower IEC than BCP_26 but slightly inferior performance, suggesting that the trend of lowering IEC to improve RDE performance did not continue further. To further evaluate the properties of the prepared copolymers, AEMWE single cell measurements at 80 °C in 1 M KOH with a 5 cm2 active area were conducted. All cells were prepared identically via direct bar coating,62 with only the binder being varied in the anode catalyst layer. For the cathode, commercial Pt/C catalyst on carbon paper was used with PiperION-A binder. For anode fabrication, the same NiFe-LDH catalyst as used as for the RDE measurements. Commercial PiperION-A, similar to M0, was selected as membrane and cathode binder, as well as for a reference anode binder system. Fig. 7 displays the cell voltage, high frequency resistance (HFR), and iR-corrected cell voltage. All single cells with copolymer binders in the anode exhibited either a similar or improved cell performance compared to the PiperION-A reference (Fig. 7 a, c, d, and f). The BCP series (Fig. 7a and c) showed a clearer distinction between each polymer. Here, the cell voltage obtained from the most hydrophilic BCP_79 was similar as for the PiperION-A reference and decreased with increasing IEC of the BCP binder. In the cell with the best performing BCP_26 a high current density of 3800 mA cm−2 at 2 V was achieved. Notably, few reports have shown significantly better performance with NiFe-based anodes.57,63–65 Compared to the device with PiperION-A as binder, the voltage of this cell was lowered by 50 mV at 1 A cm−2 and by 100 mV at 3 A cm−2. The differences among the cells prepared with the stat binders were minor, but also in this case the most hydrophobic stat_22 binder consistently outperformed the cells with more hydrophilic stat_46 and stat_73. However, BCP_26 delivered the overall best performance and a reduction of the cell voltage of 40 mV at 3 A cm−2 compared to stat_22.
The HFR of all cells (Fig. 7b,e) remained consistent in the range of 50 mΩ cm2, decreasing slightly with increasing current density. The minimal variation in HFR between the cells was in the range of reproducibility observed from previous measurements,66 indicating that the HFR is mostly dominated by the membrane and less influenced by the catalyst layer including the binder. Thus, the improvement of the cell voltage by lowering the IEC of the binder is not due to ohmic resistance of the entire MEA rather than due to improved catalyst utilization in the less swollen anode layers, which in turn is caused by the better connectivity of catalyst particles and the resulting increased electrical conductivity. This is further corroborated by the kinetic analysis of the single cell data, where the cell with BCP_26 shows an up to 20% lower Tafel slope (Fig. S15). The significant increase in performance highlights the important role of the catalyst/binder layer for efficient operation, as already known from PEM water electrolysis and fuel cells.67,68
The results from single cell testing correlated well with the trends of the RDE measurements, confirming that RDE is well-suited for straightforward catalyst and binder screening.35 With a metal loading of about 1 ± 0.1 mg cm−2, the anode layer in an operational cell is typically ∼5–10 µm62 and hence much thicker compared to the RDE layers (<1 µm). Consequently, the hydroxide conductivity of the binder is expected to be less important in a thin RDE layer compared to a thicker catalyst layer in the MEA of a single cell. This can be a further reason why the largely different RDE activities within the series of BCPs did not fully translate to the single cell level. The same argumentation explains why BCP_26 and stat_22 show very similar RDE performance but BCP_26 with significantly better hydroxide conductivity outperforms stat_22 at the single cell level (reduction of cell voltage by 40 mV at 3 A cm−2). Besides this, the overall low water uptake of both BCP_26 and stat_22 appears to be a major factor for the increase in performance in both cases.
From these results we identify the IEC as one of the most important parameters of an anode ionomer binder for AEMWE. Lowering the IEC strongly lowered WU, which is additionally almost temperature-independent for BCP_26. The low water content and resulting low swelling enabled an increase in electrical conductivity within the catalyst layer. Similar effects have been reported for the humidity-dependent electrical conductivity of a Pt/C/Nafion model electrode34 and the catalyst-loading-dependent electrical conductivity of platinum group metal-free anodes.69 In our work, the low hydration of BCP_26 led to increased catalyst utilization and in turn improved RDE and single cell performance. At this point the question of the existence of an ideal IEC arises, for which binder performance can be maximized. Efforts to use a BCP with an even lower IEC of 0.35 meq. g−1 as well as an entirely hydrophobic binder were unsuccessful due to altered solubility and incompatibility with the herein used protocols for MEA preparation (see Fig. S16 and S17). Also, the question of percolation of hydrophilic domains for fractions lower than 25% is questionable, which would deteriorate ionic transport. While hydroxide transport may not be the most important parameter for a binder, we note that a beneficial contribution of decent hydroxide transport can't be excluded neither. Nevertheless, in light of the binder stabilities reported in Fig. S14, further investigation of entirely hydrophobic binders70 appears promising.
Regarding the relationship between hydroxide conductivity, WU and performance of BCPs for AEMWE in general, it is obvious that BCP_26 features an almost ideal set of characteristics for membrane applications, provided that hydrolytic stability can be improved. This is particularly important at low hydration, where nucleophilicity of the hydroxide anion is increased.53 Further studies along these lines are underway, and cations even more stable than dimethyl piperidinium are in the spotlight.54–56,58,59
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