Dongguo
Li†
a,
Andrew R.
Motz†
b,
Chulsung
Bae
c,
Cy
Fujimoto
d,
Gaoqiang
Yang
e,
Feng-Yuan
Zhang
e,
Katherine E.
Ayers
*b and
Yu Seung
Kim
*a
aMPA-11: Materials Synthesis & Integrated Devices, Los Alamos National Laboratory, Los Alamos, NM 87545, USA. E-mail: yskim@lanl.gov
bNel Hydrogen, Wallingford, CT 06492, USA. E-mail: kayers@nelhydrogen.com
cDepartment of Chemistry and Chemical Biology, Rensselaer Polytechnic Institute, Troy, New York 12180, USA
dNanoscale Science Department, Sandia National Laboratories, Albuquerque, New Mexico 87185, USA
eDepartment of Mechanical, Aerospace & Biomedical Engineering, UT Space Institute, University of Tennessee, Knoxville, TN 37388, USA
First published on 27th April 2021
Interest in the low-cost production of clean hydrogen is growing. Anion exchange membrane water electrolyzers (AEMWEs) are considered one of the most promising sustainable hydrogen production technologies because of their ability to split water using platinum group metal-free catalysts, less expensive anode flow fields, and bipolar plates. Critical to the realization of AEMWEs is understanding the durability-limiting factors that restrict the long-term use of these devices. This article presents both durability-limiting factors and mitigation strategies for AEMWEs under three operation modes, i.e., pure water-fed (no liquid electrolyte), concentrated KOH-fed, and 1 wt% K2CO3-fed operating at a differential pressure of 100 psi. We examine extended-term behaviors of AEMWEs at the single-cell level and connect their behavior with the electrochemical, chemical, and mechanical instability of single-cell components. Finally, we discuss the pros and cons of AEMWEs under these operation modes and provide direction for long-lasting AEMWEs with highly efficient hydrogen production capabilities.
Broader contextHydrogen is an attractive energy carrier that can be stored, re-electrified on demand, and used to produce ammonia and other industrially important chemicals and materials. Currently, a majority (>95%) of hydrogen is produced from fossil fuels by steam reforming which releases massive amounts of carbon dioxide and atmospheric pollutants. Consequently, interest in hydrogen production from renewable sources such as biomass, geothermal, solar, or wind through water-splitting technology is growing. The anion exchange membrane water electrolyzer (AEMWE) is an alternative water-splitting technology to the well-established alkaline or proton exchange membrane water electrolyzers. AEMWEs use less expensive platinum group metal-free electrocatalysts like alkaline water electrolyzers, and have the capability to produce pressurized hydrogen at a high hydrogen production rate. However, the performance and durability of AEMWEs need to be significantly improved for practical use. In this article, we present the performance and durability of state-of-the-art AEMWEs. Then we discuss the durability-limiting factors of AEMWEs based on our own and other's key publications. Comprehensive degradation mechanisms and in-depth discussions on the mitigation strategies will provide future directions to develop commercially viable AEMWE systems. |
Fig. 1 Schematic single cell configurations of different water electrolyzers. (a) SOEC, (b) AWE, (c) PEMWE, and (d) AEMWE. |
For low-temperature operation (<100 °C), alkaline water electrolyzers (AWEs) are the well-established technology. AWEs use an aqueous KOH solution as a liquid electrolyte and a porous diaphragm separator (Fig. 1b). The research activity to develop platinum group metal (PGM)-free electrocatalysts for hydrogen and oxygen evolution reactions (HER and OER, respectively) is well documented.5–7 Current research is moving towards leveraging chloralkali cell configurations, e.g., the zero-gap design, to increase current density or add pressure. The hydrogen production rate of AWEs is low, typically 200 mA cm−2 at a cell voltage of 1.8 V with an energy efficiency of 75%HHV.8,9
Proton exchange membrane water electrolyzers (PEMWEs) use a proton exchange membrane (PEM) and ionomer in the electrode which allows cell operation without circulating liquid electrolytes. In this configuration, both electrodes (anode and cathode) are in physical contact with a non-porous PEM resulting in compact cell arrangements (zero-gap configuration) (Fig. 1c). This zero-gap design allows the operation of PEMWEs at ∼2 A cm−2 with an efficiency of 74%HHV.9 Besides, the non-porous membrane of PEMWEs allows for differential pressure operation which produces high-pressure hydrogen at the cathode and atmospheric pressure oxygen at the anode. Such differential pressure operations can minimize the need for second stage mechanical compression to pressurize for hydrogen storage. Despite these advantages, the high costs of the electrocatalysts, such as iridium oxide and platinum, and the corrosion-resistant current collectors and separator plates in acidic environments may become a limitation for very large systems as the cell stack becomes a larger contributor to total system cost.10 Both AWEs and PEMWEs are considered matured technologies and have been deployed at a commercial scale depending on the specific needs of the application.
Anion exchange membrane water electrolyzers (AEMWEs) operate under an alkaline environment in which PGM-free catalysts could be used. Anion exchange membranes (AEMs) are non-porous hydroxide-conducting polymers that contain immobilized, positively charged functional groups on their backbone or pendant side chains, enabling a zero-gap configuration and differential pressure operation (Fig. 1d). The overall reaction of AEMWEs consists of HER and OER. Water or alkaline liquid electrolyte is circulated through the cathode where water is reduced to hydrogen and hydroxide ions by adding two electrons from the anode (H2O + 2e− → H2 + OH−). The hydroxide ions diffuse through the AEM to the anode while the electrons are transported to the cathode through the external circuit. In the anode, the hydroxide ions recombine as oxygen and water and produce two electrons (2OH− → ½O2 + H2O + 2e−). The hydrogen and oxygen form as bubbles at the surface of the HER and OER catalysts, respectively. Similar to PEMWEs, the zero-gap configuration of AEMWEs employing a non-porous membrane can produce hydrogen at a high rate and minimize the need for mechanical hydrogen compression for storage.11 It is worth noting that AEMWEs take advantage of both AWEs (PGM-free catalyst) and PEMWEs (zero-gap configuration and non-porous membrane). Interestingly, in stark contrast to PEMWEs that use only polymer electrolytes, many AEMWEs often use liquid electrolytes (e.g., KOH or K2CO3 solutions) in addition to polymer electrolytes. A recent modeling study suggested that the additional liquid electrolyte not only reduces the ohmic resistance of the membrane and catalyst layer, but also improves the reaction kinetics.12 By adding a liquid electrolyte to the cell, the local pH increases at the catalyst–electrolyte interface and an additional electrochemical interface is generated. Industrial AEMWEs comprised of Ni-based catalysts produced hydrogen with ∼1.8 A cm−2 at 2 V in 1 M KOH which approaches the performance of conventional PEMWEs under ambient pressure.13 Due to the low-cost of catalysts and hardware, applicable zero-gap configurations, and differential pressure operation, interest in hydrogen production via AEMWEs is growing. A bibliometric analysis of the publications of AEMWEs by Journal Citation Reports (JCR) indicated that the articles’ publication number of AEMWE-related research rapidly increased over the last three years (Fig. 2), reaching 7.2% of the publication number of water electrolyzer research in 2020.
The most critical technical challenge for AEMWEs in commercially viable systems is their durability. The durability of AEMWEs normally means the longevity or lifetime of the devices. In the early stage of AEMWE development, the longevity measurement of AEMWEs is relatively easy because the lifetime of the cell is short (<500 hours). However, as more durable AEMWEs are developed, measuring the longevity of AEMWEs becomes cumbersome. Note that running a cell over 10000 hours takes more than a year. Therefore, the durability of AEMWEs has often been evaluated by the voltage change rate during an extended-term test (100–1000 hours) or by an accelerated stress test (AST) using degradation accelerating parameters such as higher operating temperatures, high current density, etc. However, one should note that extended-term tests using the voltage change rate and longevity under AST conditions cannot accurately predict the lifetime of AEMWEs because the cell lifetime is affected by the combination of several degradation modes and often limited by catastrophic failure. Therefore, it is still important to obtain the lifetime of the cell by continuously running the cell under normal operating conditions.
While the stack lifetime of commercial PEMWEs is close to 20000 to 60000 hours, the reported longevity of most AEMWEs is <3000 hours. Moreover, most AEMWEs have been tested under ambient pressure conditions. In the early stage of research, the chemical stability of AEMs under high pH conditions was regarded as the most critical durability-limiting factor of AEM-based electrochemical devices and consequently, extensive research was accordingly devoted. To date, several hydroxide-conducting polymers comprising of an alkaline-stable cationic functional group and polymer backbone, are available for AEM-based electrochemical devices.14–20 Those alkaline-stable polymers showed less than 5% loss in ion exchange capacity (IEC) even after several thousand hours in 1–4 M KOH at 80–95 °C.21,22 However, many AEM fuel cells (AEMFCs) and AEMWEs have shown a substantial reduction in performance over the first 100–200 hours of operation.23–27 These results suggest that there are other durability-limiting factors besides the alkaline instability of AEMs.
Here, we present the durability-liming factors of AEMWEs. We have structured our discussion based on the following considerations. First, when comparing the durability of AEMFCs and AEMWEs, the durability of AEMWEs seems to be better. When the same quaternized Diels–Alder poly(phenylene) AEM and ionomer were used, the lifetime of the AEMFC using the polymer was only 300 hours.28 In contrast, the lifetime of the AEMWE was more than 2000 hours.29 The higher longevity of AEMWEs is also evidenced by the fact that approximately 2000 hours of durability of AEMFCs was demonstrated recently after extensive research,30 whereas the reported lifetime of a 1 M KOH circulated AEMWE was 12000 hours even though AEMWE research was still in infancy.31 This result suggests that the durability-limiting factors for the two AEM-based devices may be different and previous articles on AEMFC durability32–34 may not cover all aspects of the AEMWE-specific degradation pathways. Second, when determining durability-limiting factors, the performance of AEMWEs needs to be considered because there are often trade-offs between performance and durability. This aspect is critical since a commercially viable AEMWE system requires both good performance as well as durability. The performance of AEMWEs using PGM-free catalysts is of particular interest as the primary benefit of AEMWEs is their ability to use PGM-free catalysts. Third, the durability of AEMWEs strongly depends on the operation mode, i.e., the type of liquid electrolyte and applied pressure level. Counterintuitively, the corrosive concentrated KOH-circulating AEMWEs showed more stable performance than pure water-fed AEMWEs which suggests that the primary durability-limiting factor may change depending on operating environments. Therefore, it is critical to address the durability-limiting factors of AEMWEs in terms of operation modes. Fourth, transient operations including start-up/stop, may affect the lifetime of AEMWEs. However, transient operations for AEMWEs are much less extensive than automotive fuel cells for which large voltage swings and frequent start-up/stops are expected.35 Since there are limited durability studies for the transient operation of AEMWEs, we herein provide the durability perspective of AEMWEs under steady-state operating conditions.
Fig. 3 explains the impact of circulating liquid electrolytes on AEMWE performance with a schematic of half-cells using hexamethyltrimethylammonium functionalized Diels–Alder poly(phenylene) (HTMA-DAPP) under pure water-fed, 1 wt% K2CO3-fed, and 1 M KOH-fed conditions. Under the pure water-fed conditions, only the polymeric material provides hydroxide conduction pathways as in the case of PEMWEs. The hydroxide conductivity (σbulk) of the AEM is 18.4 mS cm−1 at 50 °C. At the electrode, the effective conductivity (σeffective) of the ionomeric binder is calculated to 1.2 mS cm−1 from eqn (1).
(1) |
Fig. 3 Schematic illustration of a half cell with supplying pure water, 1 M KOH, or 1 wt% K2CO3 solution.12 We estimated the conductivity of AEM from the high-frequency resistance of the cell using an HTMA-DAPP AEM as a function of KOH concentration at 50 °C. |
Under the 1 M KOH-fed conditions, the conductivity of the AEM increases to 57.4 mS cm−1. At the electrode, the σeffective of the ionomeric binder and the liquid electrolyte increases to 27 mS cm−1, respectively. Note that the conductivity increase in the liquid electrolyte phase is much more significant. Adding the highly concentrated KOH solution improves the catalyst utilization five times. The improvement of the catalyst utilization is due to the expanded catalyst–electrolyte interfacial area and the improved intrinsic kinetics of the catalysts. Under the 1 wt% K2CO3-fed conditions (equivalent to 0.07 M KOH), the conductivities of the AEM and the ionomeric binder are 37 and 2.4 mS cm−1, respectively. Like the 1 M KOH-fed conditions, the added K2CO3 electrolyte (σeffective = 2.46 mS cm−1) provides an additional pathway of hydroxide conduction that contributes to increased catalyst utilization 1.5 times that of the pure water-fed conditions. As a result of the low ohmic resistance and high catalyst utilization, the performance of the liquid electrolyte-fed AEMWEs is much better than that of pure water-AEMWE. The current density of the pure water-, 1 wt% K2CO3- and 1 M KOH-fed AEMWEs at 60 °C were 450, 1200, and 1700 mA cm−2 at 2 V, respectively.
Fig. 4a and b shows the chronological progress in cell performance of pure water-fed AEMWEs employing PGM-free catalysts. The AEMWE performance of MEAs employing a PGM-free anode and PGM cathode increased from 0.2 to 0.85 A cm−2 at 2.0 V in publications from the year 2011 to 2015. Then, a substantially higher performance (>0.5 A cm−2 at 1.7 V) was obtained by 2020 and 2021 cells (Fig. 4a). The striking performance improvement is primarily due to the high IEC (∼3.3 mequiv. g−1) of the ionomer that provides a high pH environment.56 Additionally, the AEMWEs used thin membranes (thickness: 20–35 μm) and operated at high temperatures (85 and 90 °C). The AEMWE performance of MEAs employing PGM-free catalysts for both electrodes also increased from 0.24 to 1.0 A cm−2 at 1.8 V from the year 2012 to 2020 (Fig. 4b). When compared to PGM catalyzed AEMWEs (black dash line), the PGM-free AEMWEs exhibited lower performance due to the limited activity of the PGM-free cathode. The AEMWE using a PGM cathode and PGM-free anode (blue line in Fig. 4a) outperformed the PGM-catalyzed AEMWE (black dash line Fig. 4b).
Fig. 4 Selected performance of AEMWEs in the literature. (a) Pure water-fed AEMWEs with PGM-free anode/PGM cathode.57–63 Adapted with permission.58,63 Copyright 2013, IOP publishing, Copyright 2021, American Chemical Society. (b) Pure water-fed AEMWEs with PGM-free anode/PGM-free cathode.62,64–66 (c) 1 M KOH-fed AEMWEs.66–71 Adapted with permission.67–71 Copyright 2014, Elsevier, Copyright 2017, IOP Publishing, Copyright 2019, American Chemical Society, Copyright, 2020, John Wiley and Sons. (d) 1 wt% K2CO3-fed AEMWEs.72–74 Adapted with permission.72–74 Copyright 2012, 2018, Elsevier, Copyright 2014, John Wiley and Sons. The 2020 cell data was produced at Los Alamos National Laboratory. AEM: alkyl ammonium functionalized poly(styrene-b-ethylene-b-styrene) triblock copolymer (SES-TMA, 35 μm thick); anode: NiFe (4 mg cm−2); cathode: PtRu/C (50 wt% Pt, 25 wt% Ru, 2 mgPt cm−2). |
Like pure water-fed AEMWEs, the concentrated KOH-fed AEMWE performance of MEAs significantly improved over the last years (Fig. 4c). The current density of 0.1 A cm−2 at 1.8 V of the 2014 cell (dark gray line) increased to 1.0 A cm−2 for the 2019 cell (pink line). The performance of 24 wt% KOH-fed AEMWE reported in 2019 showed higher performance (1.7 A cm−2 at 2.0 V, green line), presumably due to the highly concentrated (4.4 M) KOH electrolyte. The 1.0 M KOH-fed 2020 AEMWE cell employing a commercially reinforced membrane (X37-50-T, thickness: 50 μm, Dioxide Materials) exhibited substantially higher performance (1 A cm−2 at 1.57 V, light blue line) at 80 °C with an efficiency of 75.1%HHV that was even higher than the PGM-catalyzed AEMWE (black dash line). Compared to the performance of pure water-fed AEMWEs, the performance of KOH-fed AEMWEs was notably better (0.3 A cm−2 at 1.57 V for water-fed vs. 1 A cm−2 for 1 M KOH-fed). Although no longer-term stability was reported for the 2020 cell, notable performance loss was observed over the 25 hour test at 50 °C and a constant current density of 500 mA cm−2.50
Fig. 4d shows the chronological progress of the single-cell performance of 1 wt% K2CO3-fed AEMWEs from 2014 to 2020. The performance of 1 wt% K2CO3-fed AEMWEs is relatively low. The current density of the concentrated KOH-fed AEMWEs (PGM-free electrodes) is >0.5 A cm−2 at 1.6 V (green and light blue lines in Fig. 4c), while the current density of the 1 wt% K2CO3-fed 2020 AEMWE cell (PGM-free anode) is 0.34 A cm−2 at 1.6 V (light blue line). One of the reasons for this low performance is the high cell resistance of 1 wt% K2CO3-fed AEMWEs because of their lower mobility, approximately 3–4 times in the presence of carbonate and bicarbonate ions, compared to a carbonate ion-free system.75,76
The literature survey indicates that the performance of current PGM-free catalyzed AEMWEs increases in the order: concentrated KOH-fed (Fig. 4a, light blue) ≫ pure water-fed (Fig. 4a, blue) > 1 wt% K2CO3-fed (Fig. 4b, light blue). The high performance of the concentrated KOH-fed AEMWEs is mainly due to the high pH environment. The higher performance of the SOA pure water-fed AEMWEs compared to 1 wt% K2CO3-fed AEMWEs contradicts the results shown in the electrolyte impact (Section 2.1). However, one should note that the pure water-fed AEMWE performance in literature was obtained at relatively high operating temperatures and more advanced ionomeric binders that provide a high local pH at the catalyst–electrolyte interface. Also, one should consider that other cell issues, such as soft shorts or gas mixing, may cause the very low voltages of highly-performing AEMWE cells.
The long-term performance of pure water-fed AEMWEs was reported in 2012–2014 (Fig. 5a).29,77 All three pure water-fed AEMWEs have more than 500 hours of lifetime at 50 °C and a constant current density of 200 mA cm−2. The degradation rate of the cells was relatively high because less stable AEMs and ionomers were used for the tests. The quaternized Radel® poly(sulfone) AEM used in one of the cells had an aryl ether group in the polymer backbone that is susceptible to the nucleophilic substitution, SN2, under high pH conditions. Ex situ alkaline stability of the benzyltrimethyl ammonium functionalized Diels–Alder poly(phenylene) (BTMA-DAPP) polymer indicated that the hydroxide conductivity of the polymer decreased from 13 to 1 mS cm−1 after 550 hours exposure in 0.5 M NaOH at 80 °C and 95% RH due to the SN2 of the BTMA group.15 The reported longest lifetime of the pure water-fed AEMWE under steady-state conditions is the BTMA-DAPP based AEMWE that operated 2200 hours before the test was halted due to other testing commitments. However, the voltage degradation rate of the BTMA-DAPP-based AEMWE was high, ca. 0.2 mV h−1 at the low current density. Recently, Xu et al. reported a more stable PGM catalyzed pure water-fed AEMWE at 80 °C and a constant current density of 500 mA cm−2. The cell voltage increased from 1.7 to 1.75 V after 500 hours (voltage degradation rate: 0.1 mV h−1).78 Challenges in the durability of water fed-AEMWEs include demonstrating >10000 hours of operation with higher hydrogen production rates and lower degradation rates. Demonstration of durability under differential pressure conditions remains a future task as well.
Fig. 5 Durability of AEMWEs. (a) Pure water-fed AEMWEs under ambient pressure.29 (b) 1 M KOH-fed AEMWEs at a current density of 1 A cm−2. AEM: Sustainion® Grade T or Sustainion® X37-50 (50 μm thick), anode: NiFe2O4 (1.8 mg cm−2), cathode: rainy nickel on nickel fiber paper (14.5 mg cm−2).31 Reproduced with permission.31 Copyright 2021, Elsevier. (c) Concentrated KOH-fed AEMWEs.79 Cell 1: the cell voltage was measured at 500 mA cm−2 and 80 °C with 20 wt% (3.6 M) KOH solution. AEM: PSU-PVP (120 μm thick), ionomer: Nafion, anode: Ni form; cathode: proprietary. Reproduced with permission.79 Copyright 2020, Elsevier. Cell 2: the cell voltage was measured at 300 mA cm−2 and 75 °C with 6 M KOH solution. AEM: Zirfon Perl (500 UPT AGFA) sandwiched by two pieces of polypropylene, anode: stainless steel 316L, cathode: Ra-Ni.80 (d) 1 wt% K2CO3-fed AEMWE at a current density of 500 mA cm−2 and under 100 psi differential pressure. The AEMWE cell data was produced at Nel Hydrogen. AEM: HTMA-DAPP (78 μm thick). Ionomer: Aemion, anode: Co3O4 (3 mg cm−2), cathode: Pt black (3 mg cm−2). |
Fig. 5b shows the long-term test of a 1 M KOH-fed AEMWE at the current density of 1 A cm−2 using commercial AEMs (Sustainion®) and PGM-free catalysts. The cell using Sustainion® Grade T AEM was able to operate >12000 hours with a voltage degradation rate of 0.7 μV h−1.31 The concentrated KOH-fed AEMWE cells using a non-quaternized membrane also showed stable performance (voltage degradation rate = ∼30 μV h−1) over 700 hours at 75–80 °C (Fig. 5c).79,80 Note that the AEMWE using the non-quaternized membrane requires a higher concentrated KOH solution (3.6–6 M) for a high hydrogen production rate. In the AEMWE cell with 20 wt% KOH, relatively large voltage fluctuations were observed due to the KOH concentration change suggesting that it may be critical to control the KOH concentration for highly concentrated KOH-fed systems.
The durability of 1 wt% K2CO3-fed AEMWEs was evaluated typically over 500–700 hours under 100 psi differential pressure conditions. Fig. 5d shows an 1 wt% K2CO3-fed AEMWE employing the HTMA-DAPP AEM at a constant current density of 0.5 A cm−2. The voltage decay rate at the operating temperature of 50 °C decreased over time and started to stabilize around ∼50 μV h−1 at the end of the 500 hour test. After 500 hours, the operating temperature of the cell was raised to 65 °C. The voltage of the cell dropped by ca. 50 mV, but the degradation rate increased to ∼200 μV h−1. After 200 hours of operation at 65 °C, the cell's operating temperature was returned to 50 °C to see whether the good durability at 50 °C was recoverable. The cell's voltage was higher than that of the initial 500 hour test. However, the cell was stabilized with a voltage decay rate of ∼1 μV h−1. At the end of the 750 hour test, the AEMWE did not show signs of cross cell leak or electronic-short failures, and the cell was able to run with a current of up to 2 A cm−2. Throughout the durability test, the AEMWE cell was held at 100 psi differential pressure.
A literature survey indicates that the highest longevity of AEMWEs demonstrated was obtained with 1 M KOH-fed AEMWE for 12000 hours with a degradation rate of 0.7 μV h−1. The longevity of pure water-fed and 1 wt% K2CO3-fed AEMWEs were only demonstrated for <3000 hours. The voltage degradation rate of SOA pure water-fed and 1 wt% K2CO3-fed AEMWEs are higher than that of the SOA 1 M KOH-fed AEMWE (50–200 μV h−1 over 500 to 700 hours at a constant current density of 500 mA cm−2). It is noted that the good durability of the pure water-fed AEMWE cell was obtained at a relatively high temperature (80 °C) and low operating voltage (1.7–1.75 V). In contrast, the good durability of the 1 wt% K2CO3-fed AEMWE was obtained at a lower temperature (50–65 °C) and higher operating voltage (1.9–2.0 V). The different optimum operating conditions in terms of operating temperature and cell voltage suggest that the primary durability-limiting factors for these AEMWEs with these two operation modes may be different. In the next section, firstly, we provide background information on AEMWE durability that includes cell voltage behaviors during an extended-term test of AEMWEs and the effects of bipolar plates and gas diffusion layers (GDLs) on AEMWE durability. Then we discuss the durability-limiting factors of AEMWEs with these three operation modes: pure water-fed, concentrated KOH-fed, and 1 wt% K2CO3-fed operating with differential pressure.
Fig. 6 Various voltage behaviors of AEMWEs during 100 hour extended-term test at a constant current density. |
Fig. 7 (a) Typical components in AEMWEs with AEM, bipolar plates (BPs) and gas diffusion layers (GDLs). (b) Felt-type GDL.86 Reproduced with permission.86 Copyright 2021, American Chemical Society. (c) Foam-type GDL.87 Copyright 2013, Elsevier. (d) Visualization image of trapped gas bubbles in the microfluidic chip representing a foam GDL.88 Reproduced with permission.88 Copyright 2014, Elsevier. (e) Stability test of the water electrolyzer, showing the first 10 hour stability test, removing bubbles, and then the second 6 hour stability test.89 Reproduced with permission.89 Copyright 2019, Elsevier. (f) Thin well tunable GDLs with straight pores and gradient porosity.90 Copyright 2017, Royal Society of Chemistry. |
The GDL is a porous transport layer located between the catalyst layer and the BP for transferring electron, mass and heat between the two components. Coating a GDL with catalysts results in a gas diffusion electrode (GDE) or a catalyst-coated substrate (CCS). Commonly used GDLs in AEMWEs include carbon paper or cloth, SS felt or mesh, Ti felt or foam, Ni foam, etc. (Fig. 7b and c).4 Mechanical/physical problems (e.g., over-compression, low permeability and wettability) and chemical/electrochemical failures (e.g. corrosion, erosion, and oxidation) can contribute to GDL degradation, further reducing the durability of AEMWEs. As aforementioned, since the OER condition and OH− ions lead to the corrosion of carbon materials during long-term operation, carbon GDLs can be more easily corroded than graphite BPs due to the higher concentration of OH− near the AEM. Similar to BPs, the passivation layer on SS and Ti GDLs can ensure AEMWE durability, which also leads to a high ICR. Additionally, the corrosion of metallic GDLs occurs when the voltage is above 2 V.91 Therefore, the corrosion of SS GDLs leads to the degradation of contact points between GDLs and catalyst layers causing increased MEA resistance and weak durability of AEMWEs. Although a lower operation voltage (<1.9 V) may reduce the corrosion of GDLs and improve the durability, the current density will be sacrificed, resulting in a lower hydrogen production rate.
More importantly, GDLs play an essential role in the mass transport of reactants and products. Recent studies have found that the mass transport aspect of GDLs also impacts the stability and durability of AEMWEs. During the electrolysis operation, oxygen bubbles on the anode must be removed from the GDL as soon as possible to prevent them from blocking catalyst active sites, especially at high current densities. Bazylak et al. visualized the gas bubble transport in GDLs to study how GDL geometry affects the multiphase flow in electrolyzers.88 Microscopy images showed that gas bubbles were trapped in the microfluidic chip representing a porous foam-based GDL in Fig. 7d. This can cause a greater mass transport problem in foam-based GDLs compared to felt-based GDLs. In addition, the researchers also found that the porosity, thickness, and pore diameter of GDLs greatly affect bubble accumulation in GDLs. Another study confirmed that the trapped gas or gas accumulation in GDLs greatly impacted the stability of AEMWEs, as shown in Fig. 7e.89 In the stability test of AEMWEs, catalyst-coated carbon clothes were used as GDEs, and 1 M KOH was pumped into AEMWEs with a flow rate of 60 mL min−1. In the first 10 hours (black line in Fig. 7e), slow degradation of 3 mA cm−2 h−1 was observed. Then, the power supply for the AEMWE was turned off, but the water pump kept working to pump out H2/O2 bubbles from the cell for 10 min. Interestingly, the performance of the AEMWE almost fully recovered after resuming the test (red line in Fig. 7e), and the current density returned to its initial value, indicating that the decay in the first 10 hours was due to the bubble accumulation and the blockage of water transportation in GDLs. Bubble accumulation and the resulting dehydration of catalyst layers and AEMs caused the blockage of reaction sites, starvation, and reduction on OH− conductance. This process may lead to not only short-term stability problems but also severe degradation over a longer period of time.
To the best of our knowledge, few studies have been reported on the BPs and GDLs for durable AEMWEs. Thus, more investigation is needed. Pt coated Ti BP/Pt coated Ti GDL and graphite BP/carbon paper could be used at the anode and cathode, respectively, as baseline materials to evaluate other components of AEMWEs for benchmark comparisons.62 In this way, the influence of BPs and GDLs on MEA durability could be minimized. Following the previous point, it is worth studying the contribution of GDLs and BPs to the degradation of AEMWEs to provide insights into the material selection and associated treatments of GDLs and BPs. Moreover, surface modification and structural optimization should be conducted for enhancing the mass transport and degradation resistance of GDLs. The modification and optimization processes include the followings: increasing the hydrophilicity of GDLs using chemical etching or surface coating; optimizing the GDL's structural and physical parameters by reducing pore size, producing graded pore dimensions, increasing porosity, and providing smooth surfaces; surface coating with TiN, Pt, Nb, or CrN for good corrosion resistance and low ICRs; using thin and well tunable GDLs with straight pores and gradient porosity to promote mass transport and reduce ICRs (Fig. 7f).90,92,93
Fig. 8 Performance-durability trade-off of pure water-fed AEMWEs.62 (a) Effect of IEC of ionomer on performance and (b) Effect of IEC of ionomers on extended-term performance. AEM: HTMA-DAPP (26 μm thick); anode: IrO2 (2.5 mg cm−2); cathode: NiFe nanofoam (3 mg cm−2). (c) Schematic of gas evolution at a high current density for pure water-fed and liquid electrolyte-fed AEMWEs. (d) Effect of current density on extended-term performance. AEM: SES-TMA (35 μm thick); ionomer: FLN-55; anode: IrO2 (2.5 mg cm−2); cathode: PtRu/C (50 wt% Pt, 25 wt% Ru, 2 mgPt cm−2). The AEMWE data was produced at Los Alamos National Laboratory. |
The detachment of the ionomeric binder is problematic for ionomers with a high IEC and high water uptake. These ionomers have greater dimensional change under fully hydrated conditions which weakens the adhesion of the ionomer on the catalyst's surface. The ionomer detachment by gas evolution occurs more severely in pure water-fed AEMWEs because the catalyst–electrolyte interfacial area of pure water-fed AEMWEs is relatively small. Thus, gas evolution occurs more inhomogeneously at a given current density (Fig. 8c). Since the gas permeability of polymeric materials is much lower than that of the KOH solution,95 it is difficult to remove the evolved gas fast enough from the catalyst-ionomer interface under high current operating conditions. Compared to PEMWEs, the gas bubble-induced ionomer detachment occurs more easily in AEMWEs because hydrocarbon-based quaternized ionomers have lower gas permeability,96,97 and a much lower adhesion due to their excessive swelling with water.98Fig. 8d shows the durability of pure water-fed AEMWEs as a function of the current density. The cell voltage of the AEMWE operated at 100 mA cm−2 was stable over the 100 hours while cell failure occurred within 40 hours when operating the cell at 300 mA cm−2 indicating that higher gas generation conditions are detrimental to pure water-fed AEMWEs. A similar effect was found with a nickel-iron oxyhydroxide catalyzed pure water-fed AEMWEs.63
The mitigation strategy of degradation caused by ionomer detachment is to use ionomers with a low IEC and to operate at a low operating temperature although substantially lower performance is anticipated. Alternatively, it may be plausible to develop high IEC ionomers with low to moderate water uptake. Polymer synthetic strategies to achieve low water-swollen hydrophobic ionomers include introducing multi-cations,99–102 polar interactions,103 and cross-linking.104–106 Several technical challenges in the design of high IEC ionomers with low water uptake need to be addressed. First, the conductivity of low water uptake of quaternized ionomers is low which reduces the hydrogen generation rate. Second, introducing multi-cations and polar group interactions into quaternized polymers often decreases the chemical stability of the ionomers. Third, the synthetic process of high IEC ionomers with low water uptake is likely more complex and expensive. Enhancing the robustness of the ionomeric film by a dispersing agent is another plausible approach. In general, non-aqueous dispersing agents increase chain entanglement of ionic group functionalized polymers,107,108 which provides better adhesion and mechanical robustness for the ionomer thin-film. Implementing a better dispersing agent may also produce a more uniform distribution of ionomers in the electrode making gas evolution more homogenous and improving cell stability under high current conditions. Reducing the size of catalyst nanoparticles may also help to a more uniform distribution of gas evolution reactions.
Fig. 9 (a) Schematic diagram of degradation mechanisms by electrochemical phenyl oxidation,109 hydrogenation and cation-hydroxide-water co-adsorption. (b) Short-term durability of pure water-fed La0.85Sr0.15CoO3 or IrO2 catalyzed AEMWEs. AEM: HTMA-DAPP (35 μm thick); ionomer: HTMA-DAPP; anode: La0.85Sr0.15CoO3 (2 mg cm−2) or IrO2 (1 mg cm−2); cathode: Pt/C (0.6 mgPt cm−2). The durability was measured under ambient pressure.114 (c) Chemical structure of polymer electrolytes used for phenyl oxidation study. (d) Extended-term AEMWE durability employing different AEM and ionomer combinations. AEM: HTMA-DAPP (35 μm thick) or SES-TMA (35 μm thick), ionomer: HTMA-DAPP, SES-TMA, or FLN55, anode: IrO2 (1 mg cm−2); cathode: PtRu/C (50 wt% Pt, 25 wt% Ru, 0.5 mgPt cm−2). |
Because electrochemical oxidation occurs with adsorbed phenyl groups on OER catalyst surfaces, the adsorption energy of phenyl groups on the surface of OER catalysts plays a critical role in the degradation process. The density functional theory (DFT) found that the adsorption energies of the phenyl group in BTMAOH that are parallelly oriented to the surface of iridium oxide(110) is higher (−1.2 to −2.2 eV at 1.6 V) than that of the La0.85Sr0.15CoO3 perovskite catalyst (−0.18 to −0.42 eV at 1.6 V).109 The RDE data is consistent with the calculation data that the phenyl oxidation rate on the surface of the iridium oxide is approximately three times higher than that on the surface of the perovskite catalyst. Fig. 9b shows the durability of the iridium oxide and perovskite catalyzed AEMWEs employing the HTMA-DAPP ionomer.114 The cell voltage of the iridium oxide catalyzed AEMWE rapidly increased from 1.7 to 2.1 V during the first 5 hours of operation. In contrast, the perovskite catalyzed AEMWE was stable at ∼1.8 V over 100 hours.
The mitigation strategy for the degradation caused by the electrochemical oxidation of the phenyl group is to use OER catalysts with low phenyl group adsorption energy. While the phenyl group adsorption energy on transition metal surfaces such as Pt, Pd, or Ir is relatively high,115,116 alloy catalysts can dramatically reduce the adsorption energy by changing the electronic structure in the d-band center. For example, the phenyl adsorption energy of the BTMA group parallel to the Pt(111) surface is −2.30 eV, whereas the phenyl adsorption energy of the BTMA parallel to the surface of Pt1Ru1(111) is −1.30 eV.117 As demonstrated in Fig. 8b, perovskite catalysts have minimal phenyl adsorbing surface properties which is beneficial for long-term operation without much performance loss. Furthermore, the lower pH dependency of perovskite catalysts may be beneficial to the performance of pure water-fed AEMWEs.118–120 Another approach is to use polymer electrolytes with less adsorption energy of phenyl groups. Quaternized polyolefins have lower adsorption energy than quaternized polyaromatics.121 Non-rotatable phenyl groups, such as fluorene or carbazole, have lower adsorption energy than the rotatable phenyl groups, such as biphenyl.66,122,123
The effects of electrochemical oxidation of phenyl groups on AEMWEs’ durability can be seen in Fig. 9c which compares the short-term voltage behaviors of three MEAs prepared by AEMs and ionomers with different phenyl adsorption characteristics. The first MEA was fabricated with HTMA-DAPP for both the AEM and ionomer. HTMA-DAPP has biphenyl and terphenyl units in its backbone so a high level of electrochemical oxidation of phenyl groups was expected.112,121 The second MEA was fabricated with a trimethylalkylammonium functionalized poly(styrene-b-ethylene-b-styrene) triblock copolymer (SES-TMA) AEM and HTMA-DAPP ionomer. The SES-TMA AEM has no phenyl group in its polymer backbone, and thus, a lower degree of phenyl oxidation is expected. The third MEA was fabricated with SES-TMA AEM and a quaternized poly(fluorene) ionomer (FLN55). The poly(fluorene) ionomer has a non-rotatable phenyl group that can minimize phenyl oxidation. Fig. 9d compares the durability of the MEAs employing those combinations of AEMs and ionomers. The performance of the MEA employing HTMA-DAPP for the AEM and ionomer decreased quickly during the first five hours of operation due to the phenyl oxidation of the ionomer and AEM. The MEA having SES-TMA AEM and HTMA-DAPP ionomer showed a gradual decrease over 80 hours. The slower degradation rate of the MEA is because the phenyl oxidation rate of the interdiffused SES-TMA and HTMA-DAPP phase in the electrode is lower than the HTMA-DAPP MEA. In contrast, the MEA employing SES-TMA AEM and FLN55 ionomer showed relatively stable performance over 80 hours under the same operating conditions.
Deactivation of HER electrocatalysts by hydrogenation of ionomer fragments and cumulative cation-hydroxide-water co-adsorption can impact the device's performance and durability (Fig. 9a). Although hydrogenation of the ionomeric binder at the AEMWE's cathode has not been systematically investigated at a single cell level, hydrogenation of phenyl, ketone, and alkene compounds on precious metal group catalysts is well documented.124–127 Strong adsorption of the hydroxide ion on the metal surface by cation-hydroxide-water coadsorption may lower the device's durability as well. Cumulative hydroxide adsorption can reduce water access to the catalyst's surface due to lower water solubility at the high hydroxide concentrated ionomeric layer.49,128 However, the cumulative hydroxide adsorption occurs mostly in HOR potentials, ca. 0.1 V vs. RHE129,130 and thus, the impact may be less than other ionomer poisonings.
Both durability-limiting factors of pure water-fed AEMWEs are related to the ionomeric binder. Because ionomer detachment from the surface of electrocatalysts occurs when there is a lack of adhesion and ionomer poisoning occurs with the adsorption of ionomer fragments on the surface of OER catalysts, degradation of pure water-fed AEMWEs proceeds on either degradation pathway. High durability may be possible under a low hydrogen-generating rate due to the performance-durability trade-off, suggesting that achieving high performance and durability of pure water-fed AEMWEs simultaneously may be a great technical challenge for the development of commercially viable systems.
Fig. 11 (a) 1 M KOH-fed AEMWEs at 60 °C at a current density of 1 A cm−2.131 AEM: Fumasep® FAS-50 (50 μm thick) or Sustainion® 37–50 (50 μm thick), ionomer: Nafion, anode: NiFe2O4 (2 mg cm−2); cathode: NiFeCo (2 mg cm−2). The durability was measured at 60 °C under ambient pressure. Reproduced with permission.131 Copyright 2017, Elsevier. (b) Short-term test of 1 M KOH-fed AEMWEs employing alkaline-stable AEMs. AEM/ionomer: HMT-PBI (43 μm thick)/HMT-PBI, Fumatech FAA-3 (50 μm thick)/FAA-3, anode and catalysts: Pt/C (0.5 mgPt cm−2), AEM/ionomer: SES25-TMA-1.7 (53 μm thick)/FLN-55, anode: IrO2 (1 mg cm−2); cathode: PtRu/C (50 wt% Pt, 25 wt% Ru, 0.5 mgPt cm−2). Reproduced with permission.18 Copyright 2016, Royal Society of Chemistry. |
Fig. 11b compares the 1 M KOH-fed AEMWE durability employing three different AEMs: FAA-3, hexamethyl-p-terphenyl poly(benzimidazolium) (HMT-PBI), and SES-TMA. While the AEMWE using a commercial FAA-3 AEM quickly degraded over 10 hours of operation at 60 °C and a constant current density of 20 mA cm−2, the AEMWE using an aryl ether-free HMT-PBI AEM showed a gradual performance decay at a constant current density of 25 mA cm−2 over 200 hours.146 The 1 M KOH-fed AEMWE cell employing SES-TMA AEM also showed stable performance over 400 hours. However, it is not certain that the AEMWEs using the alkaline-stable AEMs can operate for >20000 hours, as in the case of the SOA PEMWEs because some degradation of the polymer was observed under higher stress accelerated conditions. In this following section, we discuss possible degradation mechanisms of AEMs that are known as “alkaline-stable”.
Park et al. investigated the degradation pathways of the HTMA-DAPP AEM that has an aryl ether-free wholly aromatic polymer backbone and pendant alkyltrimethyl ammoniums.15 They found that a common nucleophilic methyl substitution (SN2) reaction occurred only under relatively high temperatures (>80 °C). Instead, the β-elimination (E2) reaction (also known as Hofmann elimination) was observed to occur over a prolonged period (Fig. 12a). Under 80 °C and 0.5 M NaOH conditions, degradation by β-elimination in the alkyl chain extender started to occur after 3500 hours and continued until the end of the experiment (after 11000 hours, 50% loss in hydroxide conductivity was observed). Under 80 °C and 4 M NaOH conditions, the degradation due to β-elimination started to occur at 1800 hours, and ∼40% loss in hydroxide conductivity was observed after 3500 hours. The delayed degradation via the β-elimination degradation process is consistent with other polymers with a long alkyl chain quaternary ammonium (more than four carbons in the alkyl chain linker).147,148 Fan et al. investigated the degradation behaviors of poly(arylimidazolium)s (Fig. 12b).149 The polymers with ethyl-, propyl-, and butyl-substituted side chains showed excellent alkaline stability. The chemical stability of these polymers after immersion of the AEM in 10 M KOH at 80 °C indicated that 94 to 98% of imidazolium remained intact after 240 hours in highly caustic solutions. The possible degradation mechanisms of the poly(arylimidazolium)s were evaluated with the less stable methyl-substituted poly(arylimidazolium). The 1H NMR analysis after the alkaline stability test suggested that the degradation of the AEMs occurs via both dealkylation (major) and ring-opening (minor) pathways.
Olsson et al. investigated the degradation mechanisms of poly(arylene piperidinium)s with methyl, butyl, hexyl, and octyl substitutes (Fig. 12c).18 The polymers showed no degradation under 2 M NaOH at 60 °C for 15 days. The degradation mechanisms of the polymers were investigated under harsher conditions (2 M NaOH at 90 °C for 360 hours). The study indicated that the major degradation pathway is the β-elimination in the piperidinium ring. A nucleophilic α-methyl substitution reaction was also identified for alkyl piperidinium, particularly with a higher KOH concentration.150,151 Aili et al. examined the chemical stability of polybenzimidazole (PBI) under 6 M NaOH at 85 °C for 176 days (Fig. 12d).152 The chemical structural change of the PBI was not detected after 116 days of aging, but a trace of structural change was detected after 176 days of aging. The 1H NMR analysis indicates that the base-catalyzed hydrolysis of PBI primarily occurs through a nucleophilic attack by hydroxide ions on the benzimidazole C2 position.153,154
The mitigation strategies of AEM degradation have been investigated. Pham suggested that higher alkaline stability of cyclic cation functionalized polymers may be achieved by introducing a pendant group that may reduce the ring strain and restrict conformation.16 Alternatively, alkaline-stable non-quaternized polymers can be used instead of quaternized polymers. PBIs have been extensively studied for this purpose. Kraglund et al. demonstrated the performance of 20 wt% (3.6 M) KOH-fed AEMWE cell employing poly(2,2′-(m-phenylene)-5,5-bibenzimidazole) (m-PBI).155 The cell's performance gradually decreased due to the base-catalyzed hydrolysis of amino groups in the polymer backbone. A more alkaline-stable poly(2,2′-(m-mesitylene)-5,5′-bibenzimidazole) (mes-PBI) was developed from the same research group.156 The mes-PBI membrane was stable in 0–10 wt% KOH at 88 °C for 207 days. In a 50 wt% aqueous KOH solution, the molecular weight of the mes-PBI membrane gradually decreased, suggesting that the polymer backbone degradation was initiated from the nucleophilic addition at the benzimidazolide C2 position. Although the alkaline stability of mes-PBI is superior to most quaternized polymers, one should note that the use of non-quaternized membranes requires a higher concentration of KOH solution to meet the conductivity requirement. Reasonably high performance and durability are possible with this approach when using non-quaternized polymer electrolytes.
Ayers et al. showed the mechanical property deterioration of quaternized poly(arylene ether) AEMs after being subjected to the Fenton's test for up to 5 hours.58 Visual inspection of the AEMs after the Fenton's test by optical microscopy showed surface cracking and possible AEM dissolution (Fig. 13a). The dominating reaction in the degradation processes of polyaromatics is the loss of OCH3 from the methoxy substituted compound. This mechanism is relevant to aryl ether-containing polymers such as polysulfones and polyether ketones as it can lead to bond breaking within the C–O–C connections (Fig. 13b).167 Owing to its electrophilic nature, the HO˙ radical preferentially attacks the aromatic ring near the aryl ether bond-forming phenols under high pH conditions (Fig. 13c).167 The attack of free radicals on the vulnerable carbon (carbon in para position for the trimethyl ammonium hydroxide group of vinyl benzyl chloride grafts) degrades the polymer backbone of the quaternized polystyrenes (Fig. 13d).165,168–170 Cation degradation by a radical attack on the benzyl triethyl ammonium is also depicted in Fig. 13e.171 In this mechanism, hydroxide ions attack the quaternary ammonium groups of the AEMs to produce ylides and water molecules by the abstraction of a proton from the α-carbon. Then, the oxygen molecules in the alkaline solution capture the electron of the ylides to produce superoxide anion radicals and quaternary ammonium radicals, respectively. The quaternary ammonium radicals subsequently degrade into ethylenes and tertiary amines. Mitigation strategies for electro-oxidative degradation by radical species include using an aryl ether-free polymer backbone172,173 and introducing cross-linking reactions.174,175 Radical inhibitors such as p-ethyl phenol that could protect the AEMs against the attack may be used.171
Fig. 13 (a) Optical microscopy analysis of AEM subjected to Fenton's test as a function of exposure time.58 Major polymer degradation by oxygen radical species. Adapted with permission.58 Copyright 2013, IOP publishing. (b) Aryl ether polymer backbone degradation. (c) Phenyl group degradation by formation of phenolates. (d) Polymer backbone degradation of quaternized polystyrene (e) Cationic group degradation. |
Identification of the major degradation mechanism of AEMs in a working cell can be tricky because AEM degradations can simultaneously occur in concentrated KOH-fed AEMWEs unlike ionomer poisoning and ionomer detachment found in pure water-fed AEMWEs does not occur simultaneously. However, operating parameter changes may help to identify the main degradation mechanism of AEMs. Radical-induced hydrolysis is proportional to the operating voltage, temperature, and catalysts. Alkaline instability and cross-linking are more dependent on the concentration of KOH. The degradation by cross-linking reaction occurs mostly during the first 100 hours of the test, but the degradation rate by hydroxide attack of AEMs is rather constant. Another difference in degradation behavior between pure water-fed and concentrated KOH-fed AEMWEs is the performance-durability trade-off. Because using a highly concentrated KOH electrolyte allows lower voltage operation which can reduce radical-induced AEM hydrolysis, a less clear performance-durability trade-off is observed in concentrated KOH-fed AEMWEs.
Fig. 15 (a) Catalyst degradation pathways under AEMWE operating conditions. (b) Durability of 1 M KOH-fed AEMWE at 500 mA cm−2 at 45 °C. AEM: Sustainion® X37-50, anode: CuCo-oxide on nickel form (CE-CCO), cathode: Pt/C (1 mgPt cm−2).92 Adapted with permission.92 Copyright 2020, Elsevier. |
To overcome the issue of catalyst degradation, various efforts have been made to develop effective material design strategies such as doping,192–196 surface-structure modification,197–199 and formation of protective layers on the catalyst surface.200–203 Such approaches are effective to improve catalytic activity and stability. However, one should note that the long-term stability of electrocatalysts has been evaluated mostly at a relatively small current density (10 mA cm−2).192,204–207 For concentrated KOH-fed conditions, there has been plenty of literature reviews covering the OER catalyst durability in which the actual test was often carried out in a half-cell immersed in concentrated alkaline solution. For pure water-fed or 1 wt% K2CO3-fed conditions, half-cell tests may not be a viable option, thus the durability of the OER catalysts needs to be evaluated in a AEMWE cell. In this case, device performance loss often originates from AEM and ionomer failure. Therefore, it may be difficult to dissect the cell and determine the degree of liability stemming from the catalyst degradation. In addition, the catalyst degradation may be accelerated by poisoning due to the ionomer as discussed in Section 4.1.2. For these reasons, the catalyst stability should ultimately be evaluated with an AEMWE cell under conditions such as (i) high current density, (ii) sufficiently long time (>1000 hours) and (iii) target electrolyte circulation.
Limited studies on the impact of catalysts on AEMWE durability was performed. Moderate device degradation for pure water-fed and carbonated solution-fed AEMWEs was demonstrated at a higher cell voltage (1.8–2.0 V) over several hundreds hours.208,209 The cell degradation rates of the AEMWEs were ∼0.2 mV h−1. For concentrated KOH-fed AEMWEs, the duration of most durability tests was ≤100 hours and degradation rates were higher.210–212 For example, Park et al. reported on the durability of surface-etched CuCo-oxide (CE-CCO) catalysts for OER.92 A half-cell test indicated that the CE-CCO catalyst was durable, exhibiting stable OER activity for 3600 hours at a constant current density of 20 mA cm−2. The performance of 1 M KOH-fed AEMWE employing the CE-CCO OER catalysts was reasonably good (1390 mA cm−2 at 1.8 V) at 45 °C. However, a notable voltage degradation, ca. 1 mV h−1, was observed during the 65 hours of extended-term test at a constant current density of 500 mA cm−2 (Fig. 15b). Although it was not clear that the performance decay of the AEMWEs originated only from the OER catalysts, the result suggests that a deeper analysis is needed to establish whether the high activity and stability of electrocatalysts are transferred to the device's performance and durability.
Mechanical toughness or the tensile energy of AEMs can be obtained from the area under the stress–strain curve. Herein, we consider two types of hydrocarbon AEMs that have reasonably high toughness. One is an elastomeric material like acidic PFSA membranes that have low modulus and strength but high elongation. The other is a polyaromatic membrane that has high modulus and strength but low elongation. The stress–strain curves of two representative polymers (HTMA-DAPP and SES-TMA) are compared in Fig. 16a. The tensile energy for the SES-TMA AEM was ∼30% higher than that of the HTMA-DAPP. The durability of 1 wt% K2CO3-fed AEMWEs employing the HTMA-DAPP and SES-TMA AEMs was compared at 100 psi differential pressure. The cell employing HTMA-DAPP AEM showed stable voltage during the 500 hours at a constant current density of 0.5 A cm−2 and 50 °C. In contrast, the cell employing SES-TMA did not hold the differential pressure for 500 hours (Fig. 16b). Initially, the cell held the differential pressure of ∼100 psi, but after about 200 hours, the cell could not hold the full differential pressure. The SES-TMA cell also showed more voltage fluctuation with a higher decay rate (310 μV h−1) although it still produced hydrogen until the end of the 500 hour-test. This result suggests that the AEMs having low stiffness and tensile strength would not be suitable for long-term operation under differential pressure conditions. For a membrane to withstand the challenging conditions of differential pressure operation, a stiffer (but not brittle) membrane is desirable. The quaternized SES-TMA polymer has large elongation and a relatively low yield strength. It is conceivable that such a low-stress membrane is slowly yielded under differential pressure conditions eventually leading to a membrane rupture. When a less corrosive K2CO3 liquid electrolyte is used, the main durability-limiting factor of K2CO3-fed AEMWE is associated with the differential pressure. The differential pressure holding capability may require an increase in the thickness of the AEM. However, because hydrocarbon AEMs generally have lower hydrogen gas permeability, thinner membranes and lower cell resistance, the best mitigation strategy for differential pressure operation is to use a rigid polyaromatic-based polymer instead of elastomeric polyolefin-based polymers. Other popular strategies include reinforcements,218 composites,219,220 and cross-linkings.221,222
Pure water-fed | Concentrated KOH-fed | 1 wt% K2CO3-fed, 100 psi differential pressure | |
---|---|---|---|
a PGM anode and cathode. | |||
Durability of SOA AEMWE | |||
Voltage degradation rate (μV h−1) | 100 at 0.5 A cm−2 (80 °C) | 0.7–30 at 0.3–1 A cm−2 (60–80 °C) | 1–50 at 0.5 A cm−2 (50 °C) |
Longevity demonstrated (hours) | >2000a | >12000 | >700 |
Ref. | 29 | 31, 79 and 80 | |
Durability-limiting factor (degradation behavior) | |||
Ionomer detachment (Type 1 & 4) | ++ | − | − |
Ionomer poisoning (Type 1 & 2) | ++ | + | + |
Alkaline instability (Type 1, 3, 4 & 5) | − | ++ | − |
Radical induced hydrolysis (Type 1) | + | ++ | + |
Cross-linking reaction (Type 1 & 5) | + | ++ | + |
Catalyst & degradation (Type 1) | + | + | + |
Mechanical failure (Type 1 & 5) | − | − | ++ |
The major degradation mechanisms of pure water-fed AEMWEs is related to the ionomeric binder at the electrodes. The first ionomer-related degradation is the ionomer detachment from electrocatalysts. This degradation path can be observed with ionomeric binders with a higher IEC which provide high pH environment without circulating an additional liquid electrolyte. Because ionomeric binders with high IEC generally have high water affinity, lack of adhesion of the ionomeric binders often causes ionomer detachment from the electrode that limits the durability of the cell. Ionomer detachment causes Type 1 behavior (cell voltage increase), as well as Type 4 behavior (cell voltage decrease) at a later stage. Electrochemical phenyl oxidation is the other durability-limiting factor that is related to the ionomeric binder. Electrochemical oxidation of the phenyl groups in the ionomeric binder causes a rapid voltage jump, (Type 2) as the local pH change in the electrode occurs in a relatively short time. The voltage degradation rate of SOA pure water-fed AEMWE was reported to be 100 mV h−1 which is still higher than the liquid electrolyte-fed AEMWEs suggesting that the commercial viable pure water-fed AEMWEs may not be realized in the near future. This is also partly because the complete overcoming of ionomer-related degradation pathways is technically challenging. An ionomer synthetic strategy towards high IEC with low water uptake may help to find a sweet spot for a highly performance with good durability.56,223 Completely removing phenyl groups in the anode ionomers224 can resolve the issues associated with the electrochemical oxidation of ionomer.
The concept of the concentrated KOH (pH ≥ 14)-fed AEMWEs was developed by combining traditional AWEs with the zero-gap configuration of PEMWEs. The performance stability of the concentrated KOH-fed AEMWEs was evaluated at a higher current density compared to pure water-fed AEMWEs. During a short-term test, the cell voltage behavior of extended-term tests shows a mixed pattern of Type 1 (cationic group degradation), Type 3 (electrolyte concentration change), and Type 4 (polymer backbone degradation), which makes it hard to interpret whether the cell is stable or unstable from an extended-term test. Occasionally, the cell also stops working with catastrophic failure behavior (Type 5). Since additional high pH electrolytes are available in the catalyst layer, the concentrated KOH-fed AEMWEs can largely remove the ionomer detachment and phenyl oxidation issues found in pure water-fed AEMWEs. Instead, the membrane and ionomer degradation under high pH conditions can cause performance loss over time. Compared to systems employing quaternized or non-quaternized membranes, there are trade-offs between performance and durability. When using a quaternized AEM, circulating relatively low concentrated KOH (1 M) is enough to produce high performance. When using a non-quaternized polymer, a higher concentration of KOH (3–5 M) is required for high performance. Quaternized polymers may be less stable than non-quaternized polymers under high pH conditions because the degradation of the polymer primarily starts with the cationic functional group, or the cationic functional group often triggers polymer backbone degradation. This means that alkaline stable non-quaternized polymers may survive with highly concentrated KOH solutions for only a prolonged period. The concentration of KOH also affects the selection of electrode binders. For the AEMWEs using a relatively low concentration of KOH (1 M) and a quaternized ionomeric binder may be beneficial for AEMWE performance. However, for AEMWEs using highly concentrated KOH (≥3 M), a more alkaline-stable non-quaternized ionomer such as Nafion might be used. Significant advancements of alkaline stability of polymeric materials over the past decade have allowed for the operation of concentrated KOH-fed AEMWEs using a quaternized AEM > 12000 hours of durability with a relatively low voltage degradation rate (0.7 μV h−1). For the AEMWEs using non-quaternized AEMs, more than 700 hours of durability with a low voltage degradation rate (30 μV h−1) was demonstrated. For a commercially viable system, additional performance and durability validation at a stack level is required. Moreover, the higher durability of such AEMWEs under differential pressure conditions needs to be demonstrated for an economically competitive system.
The 1 wt% K2CO3-fed AEMWEs are unique configurations for AEMWEs that increase the durability of the device at the cost of performance. Degradation behaviors of the 1 wt% K2CO3-fed AEMWEs when operating under differential pressure during an extended-term test may be more complex as different degradation limiting factors can play a role in addition to the behaviors associated with gas crossover increase (Type 1) and mechanical failure (Type 5). Although long-term performance data is limited, the durability of 1 wt% K2CO3-fed AEMWEs with differential pressure is reasonably good. The improved material stability at lower pH environments enables the accommodation of differential pressure operation. Operation of AEMWE cells under differential pressure conditions is important, especially in smaller scales, because mechanical compression is not economical for ambient pressure operation. However, operation under differential pressure conditions may narrow the AEM material choice to endure the highly pressurized conditions. Particularly, the AEMs having low stiffness and mechanical strength have limitations to hold differential pressure. The SOA 1 wt% K2CO3-fed AEMWEs exhibited reasonably good device durability (>700 hours) with a low voltage degradation rate (1–50 μV h−1). One remaining technical challenge for 1 wt% K2CO3-fed AEMWEs is performance improvement. The SOA 1 wt% K2CO3-fed AEMWE system showed relatively low performance compared to other electrolyte-fed AEMWE systems. Because of carbonation issues, a more conductive AEM and ionomer may be essential for 1 wt% K2CO3-fed AEMWE systems. This approach may be plausible to keep high durability with improved performance, as 1 wt% K2CO3 circulation provides less corrosive environments than concentrated KOH circulation. In addition, more active catalysts under the lower pH conditions are critical.
This article indicates that polymer electrolytes play a critical role in the durability AEMWEs. Over the past decade, various anion exchange polymer electrolytes have been developed for electrochemical applications and have mainly been used in AEMFCs. As AEMFCs have the major benefit of utilizing PGM-free oxygen reduction catalysts, the development of AEMFCs has been focused on automotive applications. In automotive AEMFC applications, the temperature difference between the fuel cell and the ambient is relatively small creating a significant challenge for designing a lightweight, small-size cooling system.225 Therefore, much effort has been devoted to designing highly stable polymer electrolytes at high operating temperatures (80–95 °C). In addition, the relatively high resistance of AEMs under desirable low RH conditions drives the reduction in thickness of AEMs. For AEMWE applications, the heat rejection constraint does not exist and the device operates under nearly liquid water saturated conditions. Instead, substantial benefits of differential pressure operation of AEMWEs drive the increase of AEM thickness or stiffness to withstand differential pressure. Increased resistance of thick AEMs can be compensated by using liquid electrolytes and a liquid water environment. Due to the less stringent requirements of AEMs in AEMWE applications, more AEM materials are available for AEMWEs applications. Several commercial AEMs were tested in the AEMWE mode.226 Fumatech's FAA3 AEMs are a poly(arylene ether) based material. Although an AEMWE using an unsupported FAA3 AEM showed reasonably high durability of up to 1000 hours of cell voltage cycling (1–1.8 V) at 50 °C,227 the alkaline stability of the aryl ether bond of AEMs is a concern for longer term and harsher conditions. Ionomr's AEMION AEMs, a methylated polybenzimidazole-based polymer (HMT-PBI), showed stable AEMWE performance at 1 A cm−2 at 60 °C for 150 hours.69 The AEM stability evaluation after longer-term operation of the AEMWE is still needed for the practical use of this AEM. Dioxide Materials’ Sustainion is based on poly(4-vinyl benzyl chloride-co-styrene) chemistry. Long-term stability (∼12000 hours) of AEMWEs using a PTFE-reinforced Sustainion AEM was demonstrated at 1 A cm−2 at 60 °C (see Fig. 5b).31 The high durability of the AEMWE cell may be obtained by maintaining the hydroxide conductivity by circulating KOH solution as the alkaline stability of the benzyl tetramethyl imidazolium cationic group of the polymer is low.144 Orion Polymer's m-TPN AEMs are based on aryl ether-free terphenylene-based materials.26 For this polymer, unsupported and reinforced composite membrane (Durion, Xergy) are available. The m-TPN-based AEMs are known for their excellent alkaline stability but the mechanical properties for differential pressure operation needs to be validated. No long-term performance data of AEMWEs using these AEMs are reported. Diaphragm membranes such as AGFA's Zirfon80,95 or ion-solvating membranes such as PBI79 showed good durability (see Fig. 5c) but those non-functionalized membranes can only be used with a highly concentrated KOH solution. Polyolefinic AEMs developed originally for AEMFCs228–230 need to verify their mechanical robustness, particularly under partial differential pressure conditions. Other aryl ether-free polyaromatics231–233 also have good potentials for AEMWE applications, but more characterization in a working electrolyzer cell is required.
From an industrialization perspective, it is clear that the AEMWE community has made great strides in recent years towards improved cell performance and has demonstrated the ability for performance to reach levels that would be viable compared to current PEM technology. Despite these developments, the technology still poses a much larger technical risk than the incumbent technologies (PEMWE and AWE) and the academic community will need to continue research to further derive the technology. Primary topics that, if researched, could enable commercialization are as follows: (i) a fundamental understanding of in situ failure mechanisms (ii) more studies showing durability (>100 hours) at practical current densities of >0.75 A cm−2 (ideally >1.0 A cm−2) and (iii) durability testing with earth abundant bipolar plates and porous transport layers. While degradation of individual cell components have been studied, there is a need to relate these to failure modes experienced within the cell during operation. One example of this could be proving an ex situ degradation protocol that relates to in situ failure mechanisms. Another example would be developing an in situ AST. To become cost competitive, cost models show that AEMWEs will need to operate at current densities >0.5 A cm−2 and potentially >1.0 A cm−2 even when assuming large reductions in MEA cost. At these current densities, it is common to see accelerated degradation rates. A key potential benefit of AEMWE is enabling the use of more earth abundant materials during construction. While some testing has used materials such as stainless steel and nickel, there should be more investigation into the impacts on cell durability. Furthermore, greater access to these materials would be beneficial to the community. In conclusion, a large amount of progress has been made in the field of AEMWE and the remaining challenge for the research community is improving and gaining a better understanding of AEMWE durability.
Footnote |
† Equal contributor. |
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