Thermal expansion of EB-PVD yttria stabilized zirconia

Yttria stabilized zirconia (YSZ) layers, suited for thermal barrier coatings (TBCs) in turbine engines, were produced by electron-beam physical vapour deposition (EB-PVD) on metallic (Ni-based alloys) ceramic (Al 2O 3) substrates (typically at 1000 °C) using ingot compositions of about 4 mol% Y 2O 3...

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Veröffentlicht in:Journal of the European Ceramic Society 2010-09, Vol.30 (12), p.2491-2496
Hauptverfasser: Ochrombel, R., Schneider, J., Hildmann, B., Saruhan, B.
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container_issue 12
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container_title Journal of the European Ceramic Society
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creator Ochrombel, R.
Schneider, J.
Hildmann, B.
Saruhan, B.
description Yttria stabilized zirconia (YSZ) layers, suited for thermal barrier coatings (TBCs) in turbine engines, were produced by electron-beam physical vapour deposition (EB-PVD) on metallic (Ni-based alloys) ceramic (Al 2O 3) substrates (typically at 1000 °C) using ingot compositions of about 4 mol% Y 2O 3–ZrO 2. Employing powdered samples, removed from the surface of the as-deposited YSZ layers, precision X-ray diffraction data sets were recorded between 60 and 900 °C and the lattice parameters of the metastable, tetragonal (t′) and the cubic (c) phases were refined using Rietveld's method. It was unambiguously verified that phase (c) was present in all investigated samples as a minority phase already in the as-deposited state. The thermal expansion coefficients of the tetragonal phase (t′) ( α 11 = 9.3(2) × 10 −6 K −1, α 33 = 10.8(1) × 10 −6 K −1) and the cubic phase (c) ( α 11 = 8.5(2) × 10 −6 K −1) were evaluated from the refined temperature dependent lattice parameter values of this study, and turned out to be close to each other, but significantly different from the coefficient of the monoclinic phase (m) ( α 11 = 9.0 × 10 −6 K −1, α 22 = 1.2 × 10 −6 K −1, α 33 = 11.9 × 10 −6 K −1, α 13 = 0.0 × 10 −6 K −1), which was derived from temperature dependent lattice parameter measurements published by Touloukian et al. 5 The expansion coefficient of the monoclinic phase (m) exhibited a very pronounced anisotropy in contrast to the tetragonal phases (t′) and (t). Our values for (t′) and (c) were in excellent agreement with that of other tetragonal and cubic phases from the literature with quite different Y 2O 3 contents.
doi_str_mv 10.1016/j.jeurceramsoc.2010.05.008
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Employing powdered samples, removed from the surface of the as-deposited YSZ layers, precision X-ray diffraction data sets were recorded between 60 and 900 °C and the lattice parameters of the metastable, tetragonal (t′) and the cubic (c) phases were refined using Rietveld's method. It was unambiguously verified that phase (c) was present in all investigated samples as a minority phase already in the as-deposited state. The thermal expansion coefficients of the tetragonal phase (t′) ( α 11 = 9.3(2) × 10 −6 K −1, α 33 = 10.8(1) × 10 −6 K −1) and the cubic phase (c) ( α 11 = 8.5(2) × 10 −6 K −1) were evaluated from the refined temperature dependent lattice parameter values of this study, and turned out to be close to each other, but significantly different from the coefficient of the monoclinic phase (m) ( α 11 = 9.0 × 10 −6 K −1, α 22 = 1.2 × 10 −6 K −1, α 33 = 11.9 × 10 −6 K −1, α 13 = 0.0 × 10 −6 K −1), which was derived from temperature dependent lattice parameter measurements published by Touloukian et al. 5 The expansion coefficient of the monoclinic phase (m) exhibited a very pronounced anisotropy in contrast to the tetragonal phases (t′) and (t). 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Employing powdered samples, removed from the surface of the as-deposited YSZ layers, precision X-ray diffraction data sets were recorded between 60 and 900 °C and the lattice parameters of the metastable, tetragonal (t′) and the cubic (c) phases were refined using Rietveld's method. It was unambiguously verified that phase (c) was present in all investigated samples as a minority phase already in the as-deposited state. The thermal expansion coefficients of the tetragonal phase (t′) ( α 11 = 9.3(2) × 10 −6 K −1, α 33 = 10.8(1) × 10 −6 K −1) and the cubic phase (c) ( α 11 = 8.5(2) × 10 −6 K −1) were evaluated from the refined temperature dependent lattice parameter values of this study, and turned out to be close to each other, but significantly different from the coefficient of the monoclinic phase (m) ( α 11 = 9.0 × 10 −6 K −1, α 22 = 1.2 × 10 −6 K −1, α 33 = 11.9 × 10 −6 K −1, α 13 = 0.0 × 10 −6 K −1), which was derived from temperature dependent lattice parameter measurements published by Touloukian et al. 5 The expansion coefficient of the monoclinic phase (m) exhibited a very pronounced anisotropy in contrast to the tetragonal phases (t′) and (t). 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Employing powdered samples, removed from the surface of the as-deposited YSZ layers, precision X-ray diffraction data sets were recorded between 60 and 900 °C and the lattice parameters of the metastable, tetragonal (t′) and the cubic (c) phases were refined using Rietveld's method. It was unambiguously verified that phase (c) was present in all investigated samples as a minority phase already in the as-deposited state. The thermal expansion coefficients of the tetragonal phase (t′) ( α 11 = 9.3(2) × 10 −6 K −1, α 33 = 10.8(1) × 10 −6 K −1) and the cubic phase (c) ( α 11 = 8.5(2) × 10 −6 K −1) were evaluated from the refined temperature dependent lattice parameter values of this study, and turned out to be close to each other, but significantly different from the coefficient of the monoclinic phase (m) ( α 11 = 9.0 × 10 −6 K −1, α 22 = 1.2 × 10 −6 K −1, α 33 = 11.9 × 10 −6 K −1, α 13 = 0.0 × 10 −6 K −1), which was derived from temperature dependent lattice parameter measurements published by Touloukian et al. 5 The expansion coefficient of the monoclinic phase (m) exhibited a very pronounced anisotropy in contrast to the tetragonal phases (t′) and (t). Our values for (t′) and (c) were in excellent agreement with that of other tetragonal and cubic phases from the literature with quite different Y 2O 3 contents.</abstract><pub>Elsevier Ltd</pub><doi>10.1016/j.jeurceramsoc.2010.05.008</doi><tpages>6</tpages></addata></record>
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subjects Alloys
Anisotropy
Ceramics
Cubic lattice
Lattice parameters
Phases
Thermal expansion
X-ray methods
Y 2O 3
Yttria stabilized zirconia
Zirconium dioxide
ZrO 2
title Thermal expansion of EB-PVD yttria stabilized zirconia
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