New rhenium-doped SrCo1-xRexO3-δ Perovskites Performing as Cathodes in Solid Oxide Fuel Cells

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Abstract

In the aim to stabilize novel three-dimensional perovskite oxides based upon SrCoO3-δ, we have designed and prepared SrCo1-xRexO3-δ phases (x = 0.05 and 0.10), successfully avoiding the competitive hexagonal 2H polytypes. Their performance as cathode materials in intermediate-temperature solid oxide fuel cells (IT-SOFC) has been investigated. The characterization of these oxides included X-ray (XRD) and in situ temperature-dependent neutron powder diffraction (NPD) experiments for x = 0.10. At room temperature, SrCo1-xRexO3-δ perovskites are defined in the P4/mmm space group, which corresponds to a subtle tetragonal perovskite superstructure with unit-cell parameters a = b ≈ ao, c = 2ao (ao = 3.861 and 3.868 Å, for x = 0.05 and 0.10, respectively). The crystal structure evolves above 380 °C to a simple cubic perovskite unit cell, as observed from in-situ NPD data. The electrical conductivity gave maximum values of 43.5 S·cm-1 and 51.6 S·cm-1 for x = 0.05 and x = 0.10, respectively, at 850 °C. The area specific resistance (ASR) polarization resistance determined in symmetrical cells is as low as 0.087 Ω·cm2 and 0.065 Ω·cm2 for x = 0.05 and x = 0.10, respectively, at 850 °C. In single test cells these materials generated a maximum power of around 0.6 W/cm2 at 850 °C with pure H2 as a fuel, in an electrolyte-supported configuration with La0.8Sr0.2Ga0.83Mg0.17O3-δ (LSGM) as the electrolyte. Therefore, we propose the SrCo1-xRexO3-δ (x = 0.10 and 0.05) perovskite oxides as promising candidates for cathodes in IT-SOFC.

Figures

  • Figure 1. X-ray diffraction (XRD) patterns (Cu Kα) for SrCo1-xRexO3–δ. Pristine SrCoO3–δ is indexed in the 2H hexagonal phase, while x = 0.05 and 0.10 oxides may be indexed in cubic Pm-3m symmetry.
  • Table 1. Unit-cell, structural para eters and reliability factors for SrCo0.90Re0.10O3–δ after the Rietveld refine ent in the tetragonal P4/mmm space group, Z = 2, from neutron powder diffraction (NPD) data at room temperature (RT). a = 3.8676(1) Å, c = 7.7296(4) Å, V = 115.624(8) Å3.
  • Figure 2. Observed (red crosses), calculated (black line) and difference (bottom line) NPD Rietveld profiles at RT for SrCo0.90Re0.10O3–δ at: (a) RT refined in the P4/mmm space group, and; (b) 950 °C refined in the cubic Pm-3m.
  • Table 2. Unit-cell parameters, displacement parameters and reliability factors for SrCo0.90Re0.10O3−δ in the cubic Pm-3m space group, refined from NPD data at 400, 600, 800 and 950 ◦C.
  • Figure 5. Thermal analysis in air (Thermogravimetric curve) for SrCo0.9Re0.1O3−δ.
  • Table 4. Area Specific Resistance (ASR) parameters obtained from the data fitting to the equivalent circuit shown in Figure 7 at different temperatures.
  • Table 4. Area Specific Resistance (ASR) parameters obtained from the data fitting to the equivalent circuit shown in Figure 7 at different temperatures.
  • Table 3. Area Specific Resistance (ASR) parameters o t t e ata fi ting to the equivalent circuit shown i Figure 7 at differ nt temperatures.

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APA

Troncoso, L., Gardey, M. C., Fernández-Díaz, M. T., & Alonso, J. A. (2016). New rhenium-doped SrCo1-xRexO3-δ Perovskites Performing as Cathodes in Solid Oxide Fuel Cells. Materials, 9(9). https://doi.org/10.3390/ma9090717

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