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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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 |
format | Article |
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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.</description><identifier>ISSN: 0955-2219</identifier><identifier>EISSN: 1873-619X</identifier><identifier>DOI: 10.1016/j.jeurceramsoc.2010.05.008</identifier><language>eng</language><publisher>Elsevier Ltd</publisher><subject>Alloys ; Anisotropy ; Ceramics ; Cubic lattice ; Lattice parameters ; Phases ; Thermal expansion ; X-ray methods ; Y 2O 3 ; Yttria stabilized zirconia ; Zirconium dioxide ; ZrO 2</subject><ispartof>Journal of the European Ceramic Society, 2010-09, Vol.30 (12), p.2491-2496</ispartof><rights>2010 Elsevier Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c479t-f3ee38ea6f0f4fae21b314bcc388b9dd4b479b4fba6f670d0a50c5fae39f4ccd3</citedby><cites>FETCH-LOGICAL-c479t-f3ee38ea6f0f4fae21b314bcc388b9dd4b479b4fba6f670d0a50c5fae39f4ccd3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.jeurceramsoc.2010.05.008$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3536,27903,27904,45974</link.rule.ids></links><search><creatorcontrib>Ochrombel, R.</creatorcontrib><creatorcontrib>Schneider, J.</creatorcontrib><creatorcontrib>Hildmann, B.</creatorcontrib><creatorcontrib>Saruhan, B.</creatorcontrib><title>Thermal expansion of EB-PVD yttria stabilized zirconia</title><title>Journal of the European Ceramic Society</title><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.</description><subject>Alloys</subject><subject>Anisotropy</subject><subject>Ceramics</subject><subject>Cubic lattice</subject><subject>Lattice parameters</subject><subject>Phases</subject><subject>Thermal expansion</subject><subject>X-ray methods</subject><subject>Y 2O 3</subject><subject>Yttria stabilized zirconia</subject><subject>Zirconium dioxide</subject><subject>ZrO 2</subject><issn>0955-2219</issn><issn>1873-619X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNqNkT1PwzAURS0EEqXwHyIWWFKeY8eO2aAtHxISDAWxWY7zLFylSbFTRPvrSVUGJmB6wz33Du8QckphRIGKi_lojqtgMZhFbO0ogz6AfARQ7JEBLSRLBVWv-2QAKs_TLKPqkBzFOAegEpQaEDF7w7AwdYKfS9NE3zZJ65Lpdfr0MknWXRe8SWJnSl_7DVbJxgfbNt4ckwNn6ogn33dInm-ms_Fd-vB4ez--ekgtl6pLHUNkBRrhwHFnMKMlo7y0lhVFqaqKlz1Wclf2hJBQgcnB5j3IlOPWVmxIzna7y9C-rzB2euGjxbo2DbarqGXORMGl5D15_itJhcqY5ALgbzQrmFCSw3b1cofa0MYY0Oll8AsT1pqC3hrQc_3TgN4a0JDr3kBfnuzK2H_ow2PQ0XpsLFY-oO101fr_zHwBpSyWXw</recordid><startdate>20100901</startdate><enddate>20100901</enddate><creator>Ochrombel, R.</creator><creator>Schneider, J.</creator><creator>Hildmann, B.</creator><creator>Saruhan, B.</creator><general>Elsevier Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7QQ</scope><scope>7SR</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20100901</creationdate><title>Thermal expansion of EB-PVD yttria stabilized zirconia</title><author>Ochrombel, R. ; Schneider, J. ; Hildmann, B. ; Saruhan, B.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c479t-f3ee38ea6f0f4fae21b314bcc388b9dd4b479b4fba6f670d0a50c5fae39f4ccd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>Alloys</topic><topic>Anisotropy</topic><topic>Ceramics</topic><topic>Cubic lattice</topic><topic>Lattice parameters</topic><topic>Phases</topic><topic>Thermal expansion</topic><topic>X-ray methods</topic><topic>Y 2O 3</topic><topic>Yttria stabilized zirconia</topic><topic>Zirconium dioxide</topic><topic>ZrO 2</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ochrombel, R.</creatorcontrib><creatorcontrib>Schneider, J.</creatorcontrib><creatorcontrib>Hildmann, B.</creatorcontrib><creatorcontrib>Saruhan, B.</creatorcontrib><collection>CrossRef</collection><collection>Ceramic Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of the European Ceramic Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ochrombel, R.</au><au>Schneider, J.</au><au>Hildmann, B.</au><au>Saruhan, B.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Thermal expansion of EB-PVD yttria stabilized zirconia</atitle><jtitle>Journal of the European Ceramic Society</jtitle><date>2010-09-01</date><risdate>2010</risdate><volume>30</volume><issue>12</issue><spage>2491</spage><epage>2496</epage><pages>2491-2496</pages><issn>0955-2219</issn><eissn>1873-619X</eissn><abstract>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.</abstract><pub>Elsevier Ltd</pub><doi>10.1016/j.jeurceramsoc.2010.05.008</doi><tpages>6</tpages></addata></record> |
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issn | 0955-2219 1873-619X |
language | eng |
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source | Elsevier ScienceDirect Journals |
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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