DOI:
10.1039/C8CC06802J
(Communication)
Chem. Commun., 2018,
54, 11873-11876
Single-compartment hydrogen peroxide fuel cells with poly(3,4-ethylenedioxythiophene) cathodes
Received
21st August 2018
, Accepted 25th September 2018
First published on 3rd October 2018
Abstract
Single-compartment hydrogen peroxide fuel cells have recently emerged as a promising energy conversion platform since H2O2 is a high energy-density liquid that functions as both fuel and oxidizer. Finding suitable electrocatalysts is challenging since most metallic electrodes also catalyze the disproportionation reaction of H2O2 into H2O and O2, representing a significant loss mechanism in peroxide fuel cells. Herein we demonstrate that the conducting polymer poly(3,4-ethylenedioxythiophene), PEDOT, is a versatile electrocatalyst for peroxide fuel cells without generating losses due to disproportionation. We find that PEDOT is a cathodic catalyst for reduction of peroxide to water, performing at a level on par with the best reported inorganic catalysts. Using PEDOT as the cathode and nickel as the anode material, open circuit potentials in the range of 0.5–0.6 V are possible, with power densities of 0.20–0.30 mW cm−2. We provide evidence to understand mechanistically how PEDOT functions as a catalyst for hydrogen peroxide reduction to water. The result of our efforts is a scalable hydrogen peroxide fuel cell cathode, which serves to demonstrate also the capabilities of organic semiconducting materials as electrocatalysts.
Fuel cells represent an important family of energy storage and conversion devices, with several mature technologies and well-established applications. The most prominent example is the hydrogen fuel cell, which consumes hydrogen gas as a fuel and utilizes atmospheric oxygen as an oxidizer, producing water as a byproduct. Despite its elegance, the hydrogen fuel cell has two disadvantages – the problem of storage of H2 as a gaseous fuel and the necessity of optimizing the proton-conducting separator membrane between the cathode and anode chambers to isolate the fuel from the oxidizer.1 Hydrogen peroxide fuel cells are a newer concept which retains the advantage of having a fuel cell with water as a byproduct, but with the significant feature of aqueous hydrogen peroxide as a liquid fuel and the single-compartment nature where H2O2 is both fuel and oxidizer and thus no separator is necessary.2–4 These fuel cells are part of a broader growing field of energy conversion and storage with H2O2, driven largely by improvements in photocatalytic platforms for conversion of solar energy into peroxide.5–8 In a hydrogen peroxide fuel cell, energy is produced because of the exergonic reactions of oxidation of hydrogen peroxide to produce oxygen and the reduction of hydrogen peroxide to water. If each of these half-reactions proceed on an anode and cathode, respectively, the energy contained in hydrogen peroxide can be electrochemically converted to electrical energy. Hydrogen peroxide reduction, at neutral to acidic pH values, proceeds on the cathode viaeqn (1). Oxidation at the anode proceeds viaeqn (2). The net reaction (eqn (3)) of producing water and oxygen from peroxide gives a net potential gain of 1.09 V. This is close to two well-known fuel cell systems: hydrogen fuel cells have a theoretical open circuit potential of 1.23 V and methanol fuel cells 1.21 V. | Cathode: H2O2 + 2H+ + 2e− → 2H2O (1.78 V vs. NHE) | (1) |
| Anode: H2O2 → O2 + 2H+ + 2e− (0.682 V vs. NHE) | (2) |
| Total: 2H2O2 → 2H2O + O2 (1.09 V) | (3) |
The spontaneous decomposition of peroxide into water and oxygen has been used for outer space rocket propulsion for decades, and the possibility of using peroxide in electrochemical energy conversion schemes has been theoretically envisioned for some time.9,10 The single-compartment peroxide fuel cell concept, however, has emerged only recently. The seminal example, published by Yamazaki et al. in 2008, featured an Ag cathode and Au, Pt, Pd or Ni as anode in alkaline media.11 With Pt as anode the highest current was achieved but also the highest amount of decomposition of peroxide without electricity generation (disproportionation loss). With this drawback in mind, Ni seemed to be the best solution since it had the lowest decomposition rate and moreover it is the lowest-cost metal of the tested ones. These initial peroxide fuel cells gave low open circuit voltages (VOC) of <150 mV, with maximum current densities in the range of 1–3 mA cm−2. In subsequent years, Fukuzumi and coworkers evaluated the ability of several iron-containing macrocyclic compounds to be suitable cathodic catalysts, though power density of such cells was limited to around 10 μW cm−2.12 Yamada et al. designed a fuel cell with an Ag/Ag–Pb alloy composite electrode as cathode and Au as anode in basic media. A maximum power density of 0.075 mW cm−2 at 0.065 V and an open circuit voltage of 150 mV was demonstrated.8 Substantial improvement was achieved by using prussian blue on carbon paper as a cathode and Ni or Ag as anode in acidic media. A maximum power density of 1.55 mW cm−2 and an VOC of 0.6 V was reached.13 The highest to-date power density of 4.2 mW cm−2 was reported by Yamada et al. They used a carbon-supported pyrazine bridged Fe[Me(CN)4] complex (Me = Pt or Pd) as cathode and Ni as anode. Such cells gave VOC values between 0.7 and 0.8 V.14 To-date, organic semiconductors/conductors have not been explored as catalysts in hydrogen peroxide fuel cells. We have recently found that organic semiconductors are good electrocatalysts,15 photocatalysts,16 and photoelectrocatalysts6,17 for hydrogen peroxide production, encouraging us to evaluate organic electronic materials for hydrogen peroxide fuel cells. The motivation for using conducting polymers is their low-cost and ease of processability. Lacking metals, organic electronic materials can be hypothesized to not catalyze disproportionation of peroxide. Moreover, conducting polymers like polythiophenes and polyaniline are stable in various aqueous environments, and have outstanding conductivity especially in acidic conditions. Conducting polymer formulations can swell in water, forming a three-dimensional network permeable to molecules and ions. They are therefore potentially an ideal matrix to bring together electrons and reactants and function as a 3D heterogeneous electrocatalyst for peroxide fuel cells. In this paper, we have evaluated the well-known18 commercial conducting polymer poly(3,4-ethylenedioxythiophene), or PEDOT, as an active material for peroxide single-compartment fuel cells. Our peroxide fuel cells comprise a PEDOT cathode and a nickel mesh anode, the latter being chosen since this is among the most promising anodic catalysts reported to-date.13,14 A schematic illustration showing the electrochemical redox processes on the respective electrodes is shown in Fig. 1a. The hypothesis we put forth for the operation of PEDOT as a cathodic catalyst is based on the well-established doping/dedoping redox process between PEDOT(0) and PEDOT(2+) (Fig. 1b). Neutral PEDOT will be oxidized by H2O2 to its charged bipolaronic form, which is in turn reduced back to neutral PEDOT by electrons flowing from the anode to cathode. This cycle results in the net reaction of hydrogen peroxide being reduced to water. In this study, we employed the aqueous commercial formulation of PEDOT stabilized with poly(styrene sulfonate), PSS (PH1000, Clevios™). Based on previously-published methods,19 20 mL of PH1000 was mixed with 2 V% dimethylsulfoxide and 0.5 V% (3-glycidyloxypropyl)trimethoxysilane, and afterwards ultrasonicated for 10 minutes. Then the mixture was poured into a Petri dish (∅ 8.5 cm) and stored under the fume hood overnight. Afterwards it was dried at 80 °C in the oven for 2 hours. The obtained foil was removed from the dish with a tweezer. The foil was cut with scissors into suitable pieces for electrodes, usually 2 × 5 cm. The foils consist of a dense nanofibrous network of PEDOT crystallites (Fig. 1c), which swells and expands in water. To test if PEDOT would be a suitable cathodic catalyst for a peroxide fuel cell, we measured the current–voltage characteristics of PEDOT (cathode) versus nickel (anode), in 0.05 M HCl with and without added peroxide (two-electrode device scheme as shown in Fig. 1a). This pH value was chosen since it is acidic enough to be favorable for proton coupled peroxide redox reactions but where nickel is still stable.14 In the absence of peroxide, the PEDOT/Ni electrode pair yielded an i–v characteristic with a small cathodic component attributed to oxygen reduction and an anodic peak characteristic of PEDOT oxidation (Fig. 1d). Addition of peroxide resulted in an obvious fuel cell effect, with a substantial increase in cathodic current and open circuit potential around 0.5 V. This indicates that indeed PEDOT performs as a cathodic catalyst for peroxide reduction to water.
|
| Fig. 1 (a) Schematic of the single-compartment hydrogen peroxide fuel cell. PEDOT foils function as the cathodic catalyst for peroxide reduction to water, while nickel mesh is used as the anodic catalyst throughout this work. (b) The chemical structure of PEDOT and schematic of the proposed redox cycle responsible for its action as a cathodic catalyst for H2O2 reduction. The neutral form of the polymer is oxidized by hydrogen peroxide, restoring the stable p-doped state, which is then cathodically reduced to start the cycle again. The net result is the reduction of peroxide to water. (c) SEM micrograph of a PEDOT:PSS foil. The material forms a uniform mesh with a fine nanostructure of PEDOT crystallites. (d) Current–voltage scan (50 mV s−1) of a PEDOT electrode versus nickel mesh in 0.05 M HCl. Addition of 0.1 M H2O2 gives clear fuel cell behavior. | |
To measure in detail the fuel cell performance, we conducted step chronopotentiometry scans (Fig. 2). Different current densities were maintained for 1 minute and the final potential registered. In addition to PEDOT:PSS, we tested a PEDOT:PSS composite with Prussian blue (PB) nano/microcrystals, synthesized according to the literature.20 PB is a well-known catalyst for reduction of peroxide to water, and is one of the to-date best materials as cathodes for peroxide fuel cells. PEDOT:PSS cathodes (Fig. 2a) afforded a VOC of 0.56 V and JSC of 2.0 mA cm−2, and maximum power density of 0.31 mW cm−2. The addition of PB increases the VOC to 0.64 V, very close to the previously reported value for PB on carbon in a peroxide fuel cell with a nickel anode (Fig. 2b). Current density does not improve however, remaining at 1.25 mA cm−2. Taken together, these data show that PEDOT:PSS is an efficient catalyst in its own right, as it gives an open circuit potential very close to that of PB. Step chronopotentiometry experiments were repeated for three cycles (each cycle = 12 minutes), and demonstrated constant power density for both types of samples. We conducted a chronoamperometric measurement of holding the cell at short circuit with a starting concentration of 0.1 M H2O2. Both types of PEDOT cathodes were found to discharge at similar rates, declining to about a tenth of the starting current density after 5 hours (Fig. 2c). Having established that PEDOT is a suitable cathodic catalyst for single-compartment peroxide fuel cells, we tested if it induces the nonelectrochemical disproportionation of H2O2 into water and oxygen. This is a major loss mechanism in peroxide fuel cells and an obstacle for deploying many metallic catalysts. Peroxide decomposition was quantified by measuring aliquots from test solution using the horseradish peroxidase/tetramethyl benzidine assay.6,21 We found that a 0.1 M H2O2 in 0.05 M HCl decomposes at a rate of 0.52 mM h−1. Nickel accelerated peroxide decomposition to 2.6 mM h−1. The presence of PEDOT formulations was found not only to not induce decomposition, but to actually stabilize the peroxide solution. PEDOT:PSS slowed decomposition to 0.34 mM h−1.
|
| Fig. 2 Peroxide fuel cell step-scan chronopotentiometry (CP) measurements, starting conditions 0.05 M HCl and 0.1 M H2O2; Ni mesh anode. Current was measured for 1 minute for each step. (a) CP measurement of a PEDOT:PSS cathode, (b) PEDOT:PSS + PB, (c) chronoamperometry at 0 V comparing the short circuit current over time for the respective cathodes. | |
In order to shed light on the mechanisms at play with PEDOT interacting with H2O2 in the context of familiar processes like oxygen-induced doping and oxygen reduction on PEDOT, we performed a series cyclic voltammetry experiments with and without H2O2 present (Fig. 3). In ambient conditions in 0.05 M HCl electrolyte, in the range of −0.4 to 0.8 V versus Ag/AgCl, PEDOT electrodes do not show any electrochemical activity save a relatively large capacitive current, characteristic of PEDOT:PSS.22 Purging with Ar prior to the experiment removes oxygen, which is known to contribute to p-doping of the PEDOT. This results is the appearance of quasi-reversible redox peaks between 0.2–0.4 V, attributable to the oxidation and re-reduction of PEDOT(0). This indicates that argon purging produces some quantity of neutral PEDOT by removing oxygen. Oxygen-purging of the electrolyte eliminates these redox peaks, and produces a smaller set of faradaic peaks resulting from the oxygen reduction reaction and accompanying reoxidation of oxygen reduction products. The oxygen reduction reaction on PEDOT was recently described, as was the effect of oxygen-induced doping increasing significantly the conductivity of PEDOT.23 The addition of H2O2 to a concentration of 0.1 M results in a drastic change of the cyclic voltammograms. Ambient PEDOT electrodes demonstrate a cathodic current with an onset around 0.4 V versus Ag/AgCl, signaling the reduction of H2O2 to water. Oxygen purging results in a three-fold increase in this cathodic current, which can be attributed to the effect of oxygen increasing the conductivity of PEDOT.23 Purging with Ar, however, results in a five-fold increase in the H2O2 reduction current relative to ambient conditions. This final result, taken together with the Ar-dedoping effect described above and shown in Fig. 3a, provides strong evidence that neutral PEDOT is the key species enabling the peroxide reduction reaction. These findings support the hypothesized reaction cycle proposed in Fig. 1b. Conducting polymers have a rich redox behavior and are stable in aqueous conditions, making them interesting 3D networks where electrons, ions, and reactants can meet. This approach led us to try using the archetypical conducting polymer PEDOT to see if it can participate in the redox cycle necessary to reduce hydrogen peroxide to water, critical to make cathodes for hydrogen peroxide fuel cells. These fuel cells are an interesting alternative technology to established hydrogen fuel cells, and their further development hinges on improving the performance of both cathodic and anodic catalysts. PEDOT fulfills its role as a cathodic catalyst on a level competitive with some of the best inorganic catalysts, with the benefit of not promoting peroxide disproportionation. Performance must be improved by optimizing PEDOT formulations, or by turning to other, next-generation conducting polymers. Tuning conducting polymers to become anodic catalysts for peroxide oxidation would lead to a complete “plastic” single-compartment hydrogen peroxide fuel cell. Once performance is optimized, long-term stability of conducting polymer electrodes must be carefully verified. The known stability of conducting polymer formulations in oxidizing, acidic environments speaks to them being a superior choice over metallic alternatives. Our demonstration serves as a promising first step in this direction.
|
| Fig. 3 Cyclic voltammograms (5 mV s−1) of PEDOT:PSS – GOPS under Ar purged, ambient and oxygen purged conditions: (a) 0.05 M HCl without peroxide (WO); (b) 0.05 M HCl with 0.1 M peroxide (W). | |
This work was supported by Vinnova in the framework of Treesearch.se and by the Knut and Alice Wallenberg Foundation. E. M. is grateful for support from the Erasmus+ scholarship program of the European Commission and useful discussions with G. Trimmel at TU Graz.
Conflicts of interest
There are no conflicts to declare.
Notes and references
-
S. Srinivasan, Fuel Cells From Fundamentals to Applications, Springer, New York, 2006 Search PubMed.
- S. Fukuzumi, Biochim. Biophys. Acta, Bioenerg., 2016, 1857, 604–611 CrossRef CAS PubMed.
- S. Fukuzumi and Y. Yamada, ChemElectroChem, 2016, 3, 1978–1989 CrossRef CAS.
- S. Fukuzumi, Joule, 2017, 1, 689–738 CrossRef CAS.
- K. Mase, M. Yoneda, Y. Yamada and S. Fukuzumi, Nat. Commun., 2016, 7, 11470 CrossRef CAS PubMed.
- M. Jakešová, D. H. Apaydin, M. Sytnyk, K. Oppelt, W. Heiss, N. S. Sariciftci and E. D. Głowacki, Adv. Funct. Mater., 2016, 26, 5248–5254 CrossRef.
- Y. Sun, I. Sinev, W. Ju, A. Bergmann, S. Dresp, S. Kühl, C. Spöri, H. Schmies, H. Wang, D. Bernsmeier, B. Paul, R. Schmack, R. Kraehnert, B. Roldan Cuenya and P. Strasser, ACS Catal., 2018, 8, 2844–2856 CrossRef CAS.
- Y. Yamada, Y. Fukunishi, S. Yamazaki and S. Fukuzumi, Chem. Commun., 2010, 46, 7334–7336 RSC.
- R. S. Disselkamp, Energy Fuels, 2008, 22, 2771–2774 CrossRef CAS.
- R. S. Disselkamp, Int. J. Hydrogen Energy, 2010, 35, 1049–1053 CrossRef CAS.
- S. Yamazaki, Z. Siroma, H. Senoh, T. Ioroi, N. Fujiwara and K. Yasuda, J. Power Sources, 2008, 178, 20–25 CrossRef CAS.
- S. Fukuzumi, Y. Yamada and K. D. Karlin, Electrochim. Acta, 2012, 82, 493–511 CrossRef CAS PubMed.
- S. A. Mousavi Shaegh, N.-T. Nguyen, S. M. Mousavi Ehteshami and S. H. Chan, Energy Environ. Sci., 2012, 5, 8225–8228 RSC.
- Y. Yamada, M. Yoneda and S. Fukuzumi, Inorg. Chem., 2014, 53, 1272–1274 CrossRef CAS PubMed.
- M. Warczak, M. Gryszel, M. Jakešová, V. Đerek and E. D. Głowacki, Chem. Commun., 2018, 54, 1960–1963 RSC.
- M. Gryszel, M. Sytnyk, M. Jakesova, G. Romanazzi, R. Gabrielsson, W. Heiss and E. D. Głowacki, ACS Appl. Mater. Interfaces, 2018, 10, 13253–13257 CrossRef CAS PubMed.
- M. K. Węcławski, M. Jakešová, M. Charyton, N. Demitri, B. Koszarna, K. Oppelt, S. Sariciftci, D. T. Gryko and E. D. Głowacki, J. Mater. Chem. A, 2017, 5, 20780–20788 RSC.
-
A. Elschner, S. Kirchmeyer, W. Lovenich, U. Merker and K. Reuter, PEDOT Principles and Applications of an Intrinsically Conductive Polymer, CRC Press, 2011 Search PubMed.
- P. Stadler, D. Farka, H. Coskun, E. D. Głowacki, C. Yumusak, L. M. Uiberlacker, S. Hild, L. N. Leonat, M. C. Scharber, P. Klapetek, R. Menon and N. S. Sariciftci, J. Mater. Chem. C, 2016, 4, 6982–6987 RSC.
- M. Vázquez-González, R. M. Torrente-Rodríguez, A. Kozell, A. Cecconello, S. Campuzano, J. M. Pingarron and I. Willner, Nano Lett., 2017, 17, 4958–4963 CrossRef PubMed.
- P. D. Josephy, T. Eling and R. P. Mason, J. Biol. Chem., 1982, 257, 3669–3675 CAS.
- C. M. Proctor, J. Rivnay and G. G. Malliaras, J. Polym. Sci., Part B: Polym. Phys., 2016, 1433–1436 CrossRef CAS.
- E. Mitraka, M. J. Jafari, M. Vagin, X. Liu, M. Fahlman, T. Ederth, M. Berggren, M. P. Jonsson and X. Crispin, J. Mater. Chem. A, 2017, 5, 4404–4412 RSC.
|
This journal is © The Royal Society of Chemistry 2018 |
Click here to see how this site uses Cookies. View our privacy policy here.