Lianqin
Wang
,
Jethro J.
Brink
and
John R.
Varcoe
*
Department of Chemistry, The University of Surrey, Guildford GU2 7XH, UK. E-mail: lianqin.wang@surrey.ac.uk; j.varcoe@surrey.ac.uk
First published on 9th October 2017
Anion-exchange membrane fuel cells face two challenges: performance and durability. Addressing the first, we demonstrate high performance with both O2 and CO2-free air supplies, even when using a Ag/C cathode. This was enabled by the development of a radiation-grafted anion-exchange membrane that was less than 30 μm thick when hydrated.
ETFE-[poly(ethyene-co-tetrafluoroethylene)]-based radiation-grafted (RG) AEM and AEI ionomers have previously been developed for use in AEMFCs.6–9 Following the trend set by the application of proton-exchange membranes (PEM) in proton-exchange membrane fuel cells (PEMFCs), we have investigated the use of a thinner RG-AEM in AEMFCs. This proved more problematic than originally anticipated, but a suitable supplier and grade of ETFE was recently identified (12.7 μm thick ETFE00127/1550 from Polyflon Technology Ltd, Eccleshall UK): this enabled the (more repeatable) synthesis of a sub-30 μm RG-AEM, which both underwent radiation-grafting to a satisfactory degree and was robust enough to test in an AEMFC at a temperature above 60 °C. This 12.7 μm thick Polyflon ETFE exhibited 55 MPa tensile stress at break (180% strain at break), which compares to the values 55 MPa/320% and 55 MPa/880% obtained with 25 and 50 μm ETFE films, respectively (the grade of ETFE used in prior studies and supplied by Nowofol, Germany).6,8
The ETFE-based RG-AEM discussed in this communication (designated ETFE-AEM from now on) was synthesised by subjecting the ETFE film to 30 kGy absorbed dose (using a 4.5 MeV e−-beam), grafting with vinylbenzyl chloride (VBC) monomer (dispersed in H2O), and aminating with aqueous trimethylamine (see Scheme 1 and the Experimental section in the ESI†). Table 1 summarises the key properties of the ETFE-AEM produced. Raman spectro-microscopy confirmed that the grafting and amination of VBC penetrated throughout the thickness of the ETFE-AEM (Fig. S1 in the ESI†); this explains the high conductivities achieved. The ETFE-AEM produced had a tensile stress at break of 22 MPa (220% strain at break).
a Calculated from eqn (S1) in the ESI. b Gravimetric water uptake calculated using eqn (2) in ref. 6. c Number of H2O molecules per Cl− anion calculated as: λ = WU(%)/(100 × 18.02 × IEC), where IEC is in mol g−1. d Through-plane swelling calculated using eqn (3) in ref. 6. e The Cl− anion conductivities of the fully hydrated ETFE-AEM (4-probe, in-plane measurements with the RG-AEM submerged in water) calculated using eqn (5) in ref. 6. | |
---|---|
Thickness(dry)/μm | 21 ± 1 |
Thickness(hydrated)/μm | 27 ± 1 |
Degree of grafting: DoGa (%) | 70 |
Ion-exchange capacity (IEC)/mmol g−1 | 2.11 ± 0.04 |
WUb (%) | 59 ± 9 |
λ | 16 ± 2 |
TPSd (%) | 28 ± 1 |
σ Cl(25 °C)e/mS cm−1 | 23.8 ± 1.6 |
σ Cl(70 °C)e/mS cm−1 | 57.8 ± 3.3 |
The ETFE-AEM was used to fabricate membrane electrode assemblies (MEA) with electrodes (5 cm2 geometric) containing the AEI powder (IEC = 1.26 ± 0.06 mmol g−1) developed in a prior study:9 all the electrocatalyst inks in this study contained 20%wt AEI powder and 80%wt electrocatalyst and were sprayed directly onto PTFE-treated Toray TGP-H-60 carbon paper gas diffusion substrate (Alfa Aesar, UK) using propan-1-ol/H2O mixed solvent.6 PtRu/C(Johnson Matthey UK, HiSpec 12100, 50%wt Pt and 25%wt Ru) was used as an anode electrocatalyst throughout this study as the hydrogen oxidation reaction on Pt is poorer in alkali than in acid:5,10 all anodes contained 0.6 mg cm−2 total metal loadings (= 0.4 mgPt cm−2). Pt/C(Johnson Matthey UK, HiSpec 4000, 40%wt) or Ag/C (BASF Fuel Cell Inc., 40%wt Ag) were used as the cathode electrocatalysts: 0.4 mgPt cm−2 and 1.0 mgAg cm−2 loadings were used, respectively. The MEAs were converted to the OH− forms by ion-exchange with aqueous KOH (1 mol dm−3) and then evaluated in both H2/O2 and H2/air(CO2 free) AEMFCs at 70 °C. Gas flow rates of 1 dm3 min−1 were used with no back-pressurisation: gas dew points were set at 66 °C, which equates to 84% relative humidities (RH) with a cell temperature of 70 °C. The ESI† contains more details on the preparation and AEMFC testing of the MEAs, which were carefully aligned to prior published methods.6 A cell temperature of 70 °C was selected for AMEFC testing as this was the highest temperature that could be consistently used without acute MEA failure occurring during testing.
Fig. 1 compares the H2/O2 AEMFC fuel cell performance of ETFE-AEM-based MEAs containing Pt/C and Ag/C cathodes. The Ag/C cathode yielded a peak power density of 1110 mW cm−2 (at 2400 mA cm−2), which compared favourably to the Pt/C cathode that yielded 1570 mW cm−2 (at 2800 mA cm−2): internal ohmic area resistances were 36 and 44 Ω cm2, respectively (at peak power densities). However, the open circuit voltages (OCV) were <0.95 V, which are much lower than the >1.0 V OCVs obtained with AEMFCs containing thicker ETFE-based RG-AEMs.6,8 This OCV data suggests that reasonably high gas crossover rates across the thin ETFE-AEM and that moving to even thinner ETFE-based RG-AEMs would be unwise.
Fig. 2 compares the performances of the MEA containing the Ag/C cathode supplied with either O2 or CO2-free air. The peak power density dropped to 699 mW cm−2 (at 1700 mA cm−2 and 44 mΩ cm2) when the cathode supply was switched to CO2-free air. This is still a respectable power density, especially considering the lower cost of Ag compared to Pt: Ag was only 1.7% of the price of Pt as of 11th August 2017 (US$17 g−1vs. US$980 g−1, respectively).11 Interestingly, the Ag/C cathode even outperformed the Pt/C cathode when supplied with CO2-free air at a cell temperature of 70 °C: the Pt/C cathode yielded only a peak power density of 650 mW cm−2 (at 1000 mA cm−2 and 39 mΩ cm2) due to larger apparent mass transport losses. This is clearly a phenomenon that needs to be investigated further in an extended study.
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Fig. 2 The H2 AEMFC performances at 70 °C of the ETFE-AEM with Ag/C (1.0 mgAg cm−2) cathodes supplied with either O2 (■, □) or CO2-free air (●, ○). |
In summary, we show that the use of a sub-30 μm ETFE-based radiation-grafted anion-exchange membrane leads to anion-exchange membrane fuel cell (AEMFC) performances higher than 1 W cm−2 even with the use of a Ag/C cathode electrocatalysts. This demonstrates that the performances of AEMFCs are reaching levels (especially on a cost vs. power basis) that could lead to heightened commercial interest. To move the technology further forward, we acknowledge that a harder challenge must be cracked: the search for a chemically-compatible anion-exchange membrane-ionomer combination that is both high performance and durable for >1000 h (mechanically robust, chemically stable) continues.
Footnote |
† Electronic supplementary information (ESI) available: Detailed descriptions of the anion-exchange membrane synthesis, membrane-electrode assembly preparation, and fuel cell test procedures. Additional Raman and SEM data. See DOI: 10.1039/c7cc06392j |
This journal is © The Royal Society of Chemistry 2017 |