Crystal structure and oxygen nonstoichiometry of the third-order Ruddlesden-Popper phase Pr4(Ni0.9Co0.1)3O10-δ
Crystal structure and thermal expansion of the third-order Ruddlesden-Popper phase Pr4Ni2.7Co0.3O10-δ (PNCO) were determined by high temperature X-ray powder diffraction (HT-XRD) and Rietveld analysis in the temperature range 25–600 °C in air. The thermal expansion coefficient (TEC) of PNCO is smal...
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doaj-b425f34a114947ac990d4304f0e375462021-06-27T04:39:53ZengElsevierOpen Ceramics2666-53952021-06-016100094Crystal structure and oxygen nonstoichiometry of the third-order Ruddlesden-Popper phase Pr4(Ni0.9Co0.1)3O10-δChristian Berger0Edith Bucher1Rotraut Merkle2Joachim Maier3Werner Sitte4Chair of Physical Chemistry, Montanuniversitaet Leoben, Franz-Josef-Straße 18, A-8700, Leoben, AustriaChair of Physical Chemistry, Montanuniversitaet Leoben, Franz-Josef-Straße 18, A-8700, Leoben, Austria; Corresponding author. Chair of Physical Chemistry, Montanuniversitaet Leoben, Franz-Josef-Straße 18, 8700, Leoben, Austria.Max Planck Institute for Solid State Research, Heisenbergstraße 1, D-70569, Stuttgart, GermanyMax Planck Institute for Solid State Research, Heisenbergstraße 1, D-70569, Stuttgart, GermanyChair of Physical Chemistry, Montanuniversitaet Leoben, Franz-Josef-Straße 18, A-8700, Leoben, AustriaCrystal structure and thermal expansion of the third-order Ruddlesden-Popper phase Pr4Ni2.7Co0.3O10-δ (PNCO) were determined by high temperature X-ray powder diffraction (HT-XRD) and Rietveld analysis in the temperature range 25–600 °C in air. The thermal expansion coefficient (TEC) of PNCO is smaller compared with first-order Ruddlesden-Popper phases and in excellent agreement with values of common electrolytes of solid oxide cells. HT-XRD, thermogravimetry, and differential scanning calorimetry showed a reversible phase transition at 600–650 °C. A single monoclinic (P21/a) phase occurs at 25–600 °C, while a mixture of monoclinic and tetragonal (I4/mmm) phases is found at 650–900 °C. The oxygen nonstoichiometry was determined by thermogravimetry as a function of temperature (300 ≤ T/°C ≤ 900) and oxygen partial pressure (8.3 × 10−4 ≤ pO2/bar ≤ 8.3 × 10−1). Data of the oxygen nonstoichiometry were further evaluated with respect to the partial molar enthalpy and entropy of oxygen, and the thermodynamic factor of oxygen.http://www.sciencedirect.com/science/article/pii/S2666539521000407Praseodymium nickelateThird-order Ruddlesden-Popper phaseCrystal structureDefect chemistrySolid oxide fuel cell cathodeSolid oxide electrolyser cell anode |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Christian Berger Edith Bucher Rotraut Merkle Joachim Maier Werner Sitte |
spellingShingle |
Christian Berger Edith Bucher Rotraut Merkle Joachim Maier Werner Sitte Crystal structure and oxygen nonstoichiometry of the third-order Ruddlesden-Popper phase Pr4(Ni0.9Co0.1)3O10-δ Open Ceramics Praseodymium nickelate Third-order Ruddlesden-Popper phase Crystal structure Defect chemistry Solid oxide fuel cell cathode Solid oxide electrolyser cell anode |
author_facet |
Christian Berger Edith Bucher Rotraut Merkle Joachim Maier Werner Sitte |
author_sort |
Christian Berger |
title |
Crystal structure and oxygen nonstoichiometry of the third-order Ruddlesden-Popper phase Pr4(Ni0.9Co0.1)3O10-δ |
title_short |
Crystal structure and oxygen nonstoichiometry of the third-order Ruddlesden-Popper phase Pr4(Ni0.9Co0.1)3O10-δ |
title_full |
Crystal structure and oxygen nonstoichiometry of the third-order Ruddlesden-Popper phase Pr4(Ni0.9Co0.1)3O10-δ |
title_fullStr |
Crystal structure and oxygen nonstoichiometry of the third-order Ruddlesden-Popper phase Pr4(Ni0.9Co0.1)3O10-δ |
title_full_unstemmed |
Crystal structure and oxygen nonstoichiometry of the third-order Ruddlesden-Popper phase Pr4(Ni0.9Co0.1)3O10-δ |
title_sort |
crystal structure and oxygen nonstoichiometry of the third-order ruddlesden-popper phase pr4(ni0.9co0.1)3o10-δ |
publisher |
Elsevier |
series |
Open Ceramics |
issn |
2666-5395 |
publishDate |
2021-06-01 |
description |
Crystal structure and thermal expansion of the third-order Ruddlesden-Popper phase Pr4Ni2.7Co0.3O10-δ (PNCO) were determined by high temperature X-ray powder diffraction (HT-XRD) and Rietveld analysis in the temperature range 25–600 °C in air. The thermal expansion coefficient (TEC) of PNCO is smaller compared with first-order Ruddlesden-Popper phases and in excellent agreement with values of common electrolytes of solid oxide cells. HT-XRD, thermogravimetry, and differential scanning calorimetry showed a reversible phase transition at 600–650 °C. A single monoclinic (P21/a) phase occurs at 25–600 °C, while a mixture of monoclinic and tetragonal (I4/mmm) phases is found at 650–900 °C. The oxygen nonstoichiometry was determined by thermogravimetry as a function of temperature (300 ≤ T/°C ≤ 900) and oxygen partial pressure (8.3 × 10−4 ≤ pO2/bar ≤ 8.3 × 10−1). Data of the oxygen nonstoichiometry were further evaluated with respect to the partial molar enthalpy and entropy of oxygen, and the thermodynamic factor of oxygen. |
topic |
Praseodymium nickelate Third-order Ruddlesden-Popper phase Crystal structure Defect chemistry Solid oxide fuel cell cathode Solid oxide electrolyser cell anode |
url |
http://www.sciencedirect.com/science/article/pii/S2666539521000407 |
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