Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics

Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x...
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Autor*in:	Hongsong, Zhang [verfasserIn] Lei, Shi Yongde, Zhao Gang, Li Zhenjun, Li

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2015

Schlagwörter:	ceramics coatings rare earth thermal barrier coatings thermal conductivity

Anmerkung:	© The Author(s) 2015

Übergeordnetes Werk:	Enthalten in: Journal of materials engineering and performance - New York, NY : Springer, 1992, 24(2015), 9 vom: 23. Juli, Seite 3394-3399
Übergeordnetes Werk:	volume:24 ; year:2015 ; number:9 ; day:23 ; month:07 ; pages:3394-3399

Links:	Volltext

DOI / URN:	10.1007/s11665-015-1621-z

Katalog-ID:	SPR021605874

Internformat


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245	1	0	\|a Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics
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520			\|a Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides with fluorite structure are successfully synthesized in the current study. The thermal expansion coefficient decreases with increasing content of $ ZrO_{2} $, which is higher than that of 7 wt.% yttria-stabilized zirconia (YSZ). The substitution of $ Zr^{4+} $ for $ Ce^{4+} $ reduces the thermal conductivity of $ Sm_{2} %$ Ce_{2} %$ O_{7} $ oxide. The thermal conductivity decreases from 1.69 W/m K (x = 0) to 1.22 W/m K (x = 0.3) at 1000 °C. The composition with x = 0.3 exhibits the lowest thermal conductivity at all temperatures, and the thermal conductivity of ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics was obviously lower than those of fully dense 7 wt.% YSZ. These results suggested promising potential applications of the ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics for high-temperature thermal barrier coatings.
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700	1		\|a Lei, Shi \|4 aut
700	1		\|a Yongde, Zhao \|4 aut
700	1		\|a Gang, Li \|4 aut
700	1		\|a Zhenjun, Li \|4 aut
773	0	8	\|i Enthalten in \|t Journal of materials engineering and performance \|d New York, NY : Springer, 1992 \|g 24(2015), 9 vom: 23. Juli, Seite 3394-3399 \|w (DE-627)329975447 \|w (DE-600)2048384-3 \|x 1544-1024 \|7 nnns
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856	4	0	\|u https://dx.doi.org/10.1007/s11665-015-1621-z \|z kostenfrei \|3 Volltext
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matchkey_str	article:15441024:2015----::hracnutvteadhraepninofiinsfm0g_
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publishDate	2015
allfields	10.1007/s11665-015-1621-z doi (DE-627)SPR021605874 (SPR)s11665-015-1621-z-e DE-627 ger DE-627 rakwb eng Hongsong, Zhang verfasserin aut Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2015 Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides with fluorite structure are successfully synthesized in the current study. The thermal expansion coefficient decreases with increasing content of $ ZrO_{2} $, which is higher than that of 7 wt.% yttria-stabilized zirconia (YSZ). The substitution of $ Zr^{4+} $ for $ Ce^{4+} $ reduces the thermal conductivity of $ Sm_{2} %$ Ce_{2} %$ O_{7} $ oxide. The thermal conductivity decreases from 1.69 W/m K (x = 0) to 1.22 W/m K (x = 0.3) at 1000 °C. The composition with x = 0.3 exhibits the lowest thermal conductivity at all temperatures, and the thermal conductivity of ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics was obviously lower than those of fully dense 7 wt.% YSZ. These results suggested promising potential applications of the ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics for high-temperature thermal barrier coatings. ceramics (dpeaa)DE-He213 coatings (dpeaa)DE-He213 rare earth (dpeaa)DE-He213 thermal barrier coatings (dpeaa)DE-He213 thermal conductivity (dpeaa)DE-He213 Lei, Shi aut Yongde, Zhao aut Gang, Li aut Zhenjun, Li aut Enthalten in Journal of materials engineering and performance New York, NY : Springer, 1992 24(2015), 9 vom: 23. Juli, Seite 3394-3399 (DE-627)329975447 (DE-600)2048384-3 1544-1024 nnns volume:24 year:2015 number:9 day:23 month:07 pages:3394-3399 https://dx.doi.org/10.1007/s11665-015-1621-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 24 2015 9 23 07 3394-3399
spelling	10.1007/s11665-015-1621-z doi (DE-627)SPR021605874 (SPR)s11665-015-1621-z-e DE-627 ger DE-627 rakwb eng Hongsong, Zhang verfasserin aut Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2015 Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides with fluorite structure are successfully synthesized in the current study. The thermal expansion coefficient decreases with increasing content of $ ZrO_{2} $, which is higher than that of 7 wt.% yttria-stabilized zirconia (YSZ). The substitution of $ Zr^{4+} $ for $ Ce^{4+} $ reduces the thermal conductivity of $ Sm_{2} %$ Ce_{2} %$ O_{7} $ oxide. The thermal conductivity decreases from 1.69 W/m K (x = 0) to 1.22 W/m K (x = 0.3) at 1000 °C. The composition with x = 0.3 exhibits the lowest thermal conductivity at all temperatures, and the thermal conductivity of ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics was obviously lower than those of fully dense 7 wt.% YSZ. These results suggested promising potential applications of the ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics for high-temperature thermal barrier coatings. ceramics (dpeaa)DE-He213 coatings (dpeaa)DE-He213 rare earth (dpeaa)DE-He213 thermal barrier coatings (dpeaa)DE-He213 thermal conductivity (dpeaa)DE-He213 Lei, Shi aut Yongde, Zhao aut Gang, Li aut Zhenjun, Li aut Enthalten in Journal of materials engineering and performance New York, NY : Springer, 1992 24(2015), 9 vom: 23. Juli, Seite 3394-3399 (DE-627)329975447 (DE-600)2048384-3 1544-1024 nnns volume:24 year:2015 number:9 day:23 month:07 pages:3394-3399 https://dx.doi.org/10.1007/s11665-015-1621-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 24 2015 9 23 07 3394-3399
allfields_unstemmed	10.1007/s11665-015-1621-z doi (DE-627)SPR021605874 (SPR)s11665-015-1621-z-e DE-627 ger DE-627 rakwb eng Hongsong, Zhang verfasserin aut Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2015 Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides with fluorite structure are successfully synthesized in the current study. The thermal expansion coefficient decreases with increasing content of $ ZrO_{2} $, which is higher than that of 7 wt.% yttria-stabilized zirconia (YSZ). The substitution of $ Zr^{4+} $ for $ Ce^{4+} $ reduces the thermal conductivity of $ Sm_{2} %$ Ce_{2} %$ O_{7} $ oxide. The thermal conductivity decreases from 1.69 W/m K (x = 0) to 1.22 W/m K (x = 0.3) at 1000 °C. The composition with x = 0.3 exhibits the lowest thermal conductivity at all temperatures, and the thermal conductivity of ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics was obviously lower than those of fully dense 7 wt.% YSZ. These results suggested promising potential applications of the ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics for high-temperature thermal barrier coatings. ceramics (dpeaa)DE-He213 coatings (dpeaa)DE-He213 rare earth (dpeaa)DE-He213 thermal barrier coatings (dpeaa)DE-He213 thermal conductivity (dpeaa)DE-He213 Lei, Shi aut Yongde, Zhao aut Gang, Li aut Zhenjun, Li aut Enthalten in Journal of materials engineering and performance New York, NY : Springer, 1992 24(2015), 9 vom: 23. Juli, Seite 3394-3399 (DE-627)329975447 (DE-600)2048384-3 1544-1024 nnns volume:24 year:2015 number:9 day:23 month:07 pages:3394-3399 https://dx.doi.org/10.1007/s11665-015-1621-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 24 2015 9 23 07 3394-3399
allfieldsGer	10.1007/s11665-015-1621-z doi (DE-627)SPR021605874 (SPR)s11665-015-1621-z-e DE-627 ger DE-627 rakwb eng Hongsong, Zhang verfasserin aut Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2015 Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides with fluorite structure are successfully synthesized in the current study. The thermal expansion coefficient decreases with increasing content of $ ZrO_{2} $, which is higher than that of 7 wt.% yttria-stabilized zirconia (YSZ). The substitution of $ Zr^{4+} $ for $ Ce^{4+} $ reduces the thermal conductivity of $ Sm_{2} %$ Ce_{2} %$ O_{7} $ oxide. The thermal conductivity decreases from 1.69 W/m K (x = 0) to 1.22 W/m K (x = 0.3) at 1000 °C. The composition with x = 0.3 exhibits the lowest thermal conductivity at all temperatures, and the thermal conductivity of ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics was obviously lower than those of fully dense 7 wt.% YSZ. These results suggested promising potential applications of the ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics for high-temperature thermal barrier coatings. ceramics (dpeaa)DE-He213 coatings (dpeaa)DE-He213 rare earth (dpeaa)DE-He213 thermal barrier coatings (dpeaa)DE-He213 thermal conductivity (dpeaa)DE-He213 Lei, Shi aut Yongde, Zhao aut Gang, Li aut Zhenjun, Li aut Enthalten in Journal of materials engineering and performance New York, NY : Springer, 1992 24(2015), 9 vom: 23. Juli, Seite 3394-3399 (DE-627)329975447 (DE-600)2048384-3 1544-1024 nnns volume:24 year:2015 number:9 day:23 month:07 pages:3394-3399 https://dx.doi.org/10.1007/s11665-015-1621-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 24 2015 9 23 07 3394-3399
allfieldsSound	10.1007/s11665-015-1621-z doi (DE-627)SPR021605874 (SPR)s11665-015-1621-z-e DE-627 ger DE-627 rakwb eng Hongsong, Zhang verfasserin aut Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2015 Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides with fluorite structure are successfully synthesized in the current study. The thermal expansion coefficient decreases with increasing content of $ ZrO_{2} $, which is higher than that of 7 wt.% yttria-stabilized zirconia (YSZ). The substitution of $ Zr^{4+} $ for $ Ce^{4+} $ reduces the thermal conductivity of $ Sm_{2} %$ Ce_{2} %$ O_{7} $ oxide. The thermal conductivity decreases from 1.69 W/m K (x = 0) to 1.22 W/m K (x = 0.3) at 1000 °C. The composition with x = 0.3 exhibits the lowest thermal conductivity at all temperatures, and the thermal conductivity of ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics was obviously lower than those of fully dense 7 wt.% YSZ. These results suggested promising potential applications of the ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics for high-temperature thermal barrier coatings. ceramics (dpeaa)DE-He213 coatings (dpeaa)DE-He213 rare earth (dpeaa)DE-He213 thermal barrier coatings (dpeaa)DE-He213 thermal conductivity (dpeaa)DE-He213 Lei, Shi aut Yongde, Zhao aut Gang, Li aut Zhenjun, Li aut Enthalten in Journal of materials engineering and performance New York, NY : Springer, 1992 24(2015), 9 vom: 23. Juli, Seite 3394-3399 (DE-627)329975447 (DE-600)2048384-3 1544-1024 nnns volume:24 year:2015 number:9 day:23 month:07 pages:3394-3399 https://dx.doi.org/10.1007/s11665-015-1621-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 24 2015 9 23 07 3394-3399
language	English
source	Enthalten in Journal of materials engineering and performance 24(2015), 9 vom: 23. Juli, Seite 3394-3399 volume:24 year:2015 number:9 day:23 month:07 pages:3394-3399
sourceStr	Enthalten in Journal of materials engineering and performance 24(2015), 9 vom: 23. Juli, Seite 3394-3399 volume:24 year:2015 number:9 day:23 month:07 pages:3394-3399
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	ceramics coatings rare earth thermal barrier coatings thermal conductivity
isfreeaccess_bool	true
container_title	Journal of materials engineering and performance
authorswithroles_txt_mv	Hongsong, Zhang @@aut@@ Lei, Shi @@aut@@ Yongde, Zhao @@aut@@ Gang, Li @@aut@@ Zhenjun, Li @@aut@@
publishDateDaySort_date	2015-07-23T00:00:00Z
hierarchy_top_id	329975447
id	SPR021605874
language_de	englisch
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author	Hongsong, Zhang
spellingShingle	Hongsong, Zhang misc ceramics misc coatings misc rare earth misc thermal barrier coatings misc thermal conductivity Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics
authorStr	Hongsong, Zhang
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topic_title	Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics ceramics (dpeaa)DE-He213 coatings (dpeaa)DE-He213 rare earth (dpeaa)DE-He213 thermal barrier coatings (dpeaa)DE-He213 thermal conductivity (dpeaa)DE-He213
topic	misc ceramics misc coatings misc rare earth misc thermal barrier coatings misc thermal conductivity
topic_unstemmed	misc ceramics misc coatings misc rare earth misc thermal barrier coatings misc thermal conductivity
topic_browse	misc ceramics misc coatings misc rare earth misc thermal barrier coatings misc thermal conductivity
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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hierarchy_parent_title	Journal of materials engineering and performance
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title	Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics
ctrlnum	(DE-627)SPR021605874 (SPR)s11665-015-1621-z-e
title_full	Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics
author_sort	Hongsong, Zhang
journal	Journal of materials engineering and performance
journalStr	Journal of materials engineering and performance
lang_code	eng
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container_start_page	3394
author_browse	Hongsong, Zhang Lei, Shi Yongde, Zhao Gang, Li Zhenjun, Li
container_volume	24
format_se	Elektronische Aufsätze
author-letter	Hongsong, Zhang
doi_str_mv	10.1007/s11665-015-1621-z
title_sort	thermal conductivities and thermal expansion coefficients of ($ sm_{0.5} %$ gd_{0.5} $)2($ ce_{1−x} %$ zr_{x} $)2$ o_{7} $ ceramics
title_auth	Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics
abstract	Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides with fluorite structure are successfully synthesized in the current study. The thermal expansion coefficient decreases with increasing content of $ ZrO_{2} $, which is higher than that of 7 wt.% yttria-stabilized zirconia (YSZ). The substitution of $ Zr^{4+} $ for $ Ce^{4+} $ reduces the thermal conductivity of $ Sm_{2} %$ Ce_{2} %$ O_{7} $ oxide. The thermal conductivity decreases from 1.69 W/m K (x = 0) to 1.22 W/m K (x = 0.3) at 1000 °C. The composition with x = 0.3 exhibits the lowest thermal conductivity at all temperatures, and the thermal conductivity of ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics was obviously lower than those of fully dense 7 wt.% YSZ. These results suggested promising potential applications of the ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics for high-temperature thermal barrier coatings. © The Author(s) 2015
abstractGer	Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides with fluorite structure are successfully synthesized in the current study. The thermal expansion coefficient decreases with increasing content of $ ZrO_{2} $, which is higher than that of 7 wt.% yttria-stabilized zirconia (YSZ). The substitution of $ Zr^{4+} $ for $ Ce^{4+} $ reduces the thermal conductivity of $ Sm_{2} %$ Ce_{2} %$ O_{7} $ oxide. The thermal conductivity decreases from 1.69 W/m K (x = 0) to 1.22 W/m K (x = 0.3) at 1000 °C. The composition with x = 0.3 exhibits the lowest thermal conductivity at all temperatures, and the thermal conductivity of ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics was obviously lower than those of fully dense 7 wt.% YSZ. These results suggested promising potential applications of the ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics for high-temperature thermal barrier coatings. © The Author(s) 2015
abstract_unstemmed	Abstract The ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides were prepared by solid-state reaction, and their phase compositions, microstructures, and thermophysical properties were investigated. Results of x-ray diffraction reveal that pure ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ oxides with fluorite structure are successfully synthesized in the current study. The thermal expansion coefficient decreases with increasing content of $ ZrO_{2} $, which is higher than that of 7 wt.% yttria-stabilized zirconia (YSZ). The substitution of $ Zr^{4+} $ for $ Ce^{4+} $ reduces the thermal conductivity of $ Sm_{2} %$ Ce_{2} %$ O_{7} $ oxide. The thermal conductivity decreases from 1.69 W/m K (x = 0) to 1.22 W/m K (x = 0.3) at 1000 °C. The composition with x = 0.3 exhibits the lowest thermal conductivity at all temperatures, and the thermal conductivity of ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics was obviously lower than those of fully dense 7 wt.% YSZ. These results suggested promising potential applications of the ($ Sm_{0.5} %$ Gd_{0.5} $)2 ($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ ceramics for high-temperature thermal barrier coatings. © The Author(s) 2015
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container_issue	9
title_short	Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics
url	https://dx.doi.org/10.1007/s11665-015-1621-z
remote_bool	true
author2	Lei, Shi Yongde, Zhao Gang, Li Zhenjun, Li
author2Str	Lei, Shi Yongde, Zhao Gang, Li Zhenjun, Li
ppnlink	329975447
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hochschulschrift_bool	false
doi_str	10.1007/s11665-015-1621-z
up_date	2024-07-03T23:33:45.598Z
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Thermal Conductivities and Thermal Expansion Coefficients of ($ Sm_{0.5} %$ Gd_{0.5} $)2($ Ce_{1−x} %$ Zr_{x} $)2$ O_{7} $ Ceramics

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