Electrochemical characterization of Pr2CuO4 cathode for IT-SOFC
Graphical abstract
Highlights
► Pr2CuO4 shows a chemical stability with respect to Ce0.9Gd0.1O1.95 up to 1173 K. ► The electrochemical behavior of Pr2CuO4 electrode was investigated. ► The rate-determining steps of ORR depend on temperature and oxygen partial pressure. ► Electrode resistance of Pr2CuO4 was stable after several thermocycles.
Introduction
Mixed electronic and ionic conductors with layered structures are presently regarded as promising cathode materials for intermediate temperature solid oxide fuel cells (IT-SOFCs) operated at 773–973 K [1], [2], [3], [4], [5]. Among them, rare-earth (RE) nickelates and cuprates RE2MO4, M = Ni and Cu attract much practical interest [2], [3], [4], [5], [6], [7], [8], [9], [10], [11]. They exhibit relatively high electrical conductivity, which depends on the nature of rare-earth cation and varies in the range of 10–100 S/cm at 773–1173 K [12], [13], [14], [15], [16], [17], [18]. Moreover, RE2MO4, M = Ni and Cu with K2NiF4 structure show high values of oxygen diffusion and surface exchange rate due to the possibility of incorporation of excess interstitial oxygen into the structure [4], [12], [13], [14], [15], [16], [18]. Relatively low polarization resistances of porous nickelates and cuprates electrode layers deposited onto solid electrolyte are acceptable for their use as cathode materials in SOFC [2], [3], [4], [5], [6], [7], [8], [9], [10], [11], [16]. Despite reduced thermodynamic stability of Pr2NiO4 in comparison with La2NiO4 and Nd2NiO4 (e.g. Pr2NiO4 decomposes at T > 1123 K in oxidizing atmosphere into Pr4Ni3O10−δ and PrOx [19]), it is widely studied as cathode material in SOFC due to both high electrical conductivity [13], [15], [16], [17], [18] and electrochemical activity for oxygen reduction [7], [15], [16]. Thermal expansion coefficients (TECs) of praseodymium nickelates and cuprates (∼12–13 × 10−6 K−1) [13], [16], [18] are comparable with ceria solid electrolyte (for Ce0.9Gd0.1O1.95 TEC = 12.4 × 10−6 K−1) [20]. It should be mentioned here that RE2NiO4 and La2CuO4 have K2NiF4-type structure (T-phase), which can be described as a sequence of perovskite layers alternating with RE2O2 slabs having rock-salt structure (Fig. 1a). However, RE2CuO4 cuprates with other than RE = La cations, in particular Pr2CuO4, possess so-called T′-phase structure with RE2O2 slabs having fluorite structure (Fig. 1b) [21]. Recently some of us showed that “compressed” RE2O2 slabs in the T′-phase lead to a smaller separation between available empty oxygen octahedral sites and RE cations and hamper oxygen anion diffusion [18]. Despite detailed investigation of the electrochemical behavior of Pr2NiO4 electrodes [7], [16], no studies of Pr2CuO4 electrodes are available to our knowledge.
In the present work we prepared Pr2CuO4 (PCO) electrodes on CGO (Ce0.9Gd0.1O1.95) electrolyte by screen-printing and report on the impedance spectroscopy study of the symmetrical cells PCO/CGO/PCO at 773–1173 K and partial oxygen pressure () 10−4–1 atm.
Section snippets
Experimental
Pr2CuO4 (PCO) powder sample was prepared by annealing of the stoichiometric mixtures of Pr6O11 (“analytical grade”) and CuO open to air at 1273 K, 20 h. Copper oxide was prepared by decomposition of (CuOH)2CO3 at 573 K. Oxygen content of PCO was determined by iodometric titration.
Phase composition of the samples was determined at room temperature by the X-ray powder diffraction (XRPD) recorded in Huber G670 Guinier diffractometer (CuKα1 radiation, image foil detector, 10° ≤ 2Θ ≤ 100°). Particle
Results and discussion
XRPD data for PCO powder after sintering at 1273 K for 20 h in air showed the formation of the single-phase material with the unit cell a = 3.958(3) Å, c = 12.210(1) Å (space group I4/mmm), which is in good agreement with the literature data for Pr2CuO4 [13], [21] (Fig. 2A). Oxygen content of the sample, determined by the iodometric titration, corresponds within e.s.d. to the stoichiometric composition.
Particle size distribution of the PCO powder is shown in Fig. 3. The majority of the
Conclusions
The electrochemical behavior of PCO electrode screen-printed on CGO electrolyte was systematically studied. TGA and XRPD measurements indicate that PCO is stable both in air and Ar at 298–1173 K. XRPD of PCO–CGO mixture after heat treatment at 1173 K for 100 h in air showed no indications of chemical interaction between materials. The impedance measurements of the PCO/CGO/PCO symmetric cell revealed that depending on temperature and oxygen partial pressure different rate-determining steps of
Acknowledgments
This work was partially supported by Ministry of Science and Education of Russian Federation (State contracts 14.740.12.1358 and 14.740.11.0033), Russian Foundation for Basic Research (Grant No. 11-08-01159a and 11-03-01225) and MSU-development Program up to 2020.
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2021, Acta MaterialiaCitation Excerpt :Since the discovery of unusual high-temperature superconductivity in the (La,Sr)2CuO4+δ family, broad interest in rare earth metal cuprates (RE2CuO4 and higher order cuprates, RE = rare earth) has led to the investigation of their fundamental materials properties [1–10]. At elevated temperatures, the rare earth cuprates, along with nickelates and cobaltates, exhibit high oxygen diffusivities and, as a result, mixed ionic and electronic conductivity (MIEC) [11–16]. Oxides with high levels of mixed conductivity, specifically with high ionic conductivity, are known to support high oxygen surface exchange rates, a key measure of performance in solid oxide fuel cell (SOFC) cathodes [17,18].
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2019, International Journal of Hydrogen EnergyCitation Excerpt :The oxygen loss is negligible (0.2% weight) in entire temperature range of measurement for PSCO-0.0, which is in agreement with reporting in the literature [35]. Lyskov et al. [30] have also reported only 0.2% weight reduction for PSCO-0.0. It has been understood that the presence of only square coordinated (coordination number (CN) = 4) Cu2+ in the crystal structure of T′-phase (PSCO-0.0) on one hand hinders further decrease of its CN and on the other hand, tightly links oxygen atoms of Pr2O2 fluorite slabs to Pr3+.