Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass
Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8...
Ausführliche Beschreibung
Autor*in: |
Döhler, Franziska [verfasserIn] Zscheckel, Tilman [verfasserIn] Kasch, Susanne [verfasserIn] Schmidt, Thomas [verfasserIn] Rüssel, Christian [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2017 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: Journal of materials science - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966, 52(2017), 16 vom: 04. Mai, Seite 9344-9354 |
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Übergeordnetes Werk: |
volume:52 ; year:2017 ; number:16 ; day:04 ; month:05 ; pages:9344-9354 |
Links: |
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DOI / URN: |
10.1007/s10853-017-1151-1 |
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Katalog-ID: |
SPR013923021 |
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245 | 1 | 0 | |a Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass |
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520 | |a Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. The resulting coefficients of thermal expansion fit well to that of $ Al_{2} %$ O_{3} $. | ||
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700 | 1 | |a Zscheckel, Tilman |e verfasserin |4 aut | |
700 | 1 | |a Kasch, Susanne |e verfasserin |4 aut | |
700 | 1 | |a Schmidt, Thomas |e verfasserin |4 aut | |
700 | 1 | |a Rüssel, Christian |e verfasserin |4 aut | |
773 | 0 | 8 | |i Enthalten in |t Journal of materials science |d Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 |g 52(2017), 16 vom: 04. Mai, Seite 9344-9354 |w (DE-627)315293969 |w (DE-600)2015305-3 |x 1573-4803 |7 nnns |
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10.1007/s10853-017-1151-1 doi (DE-627)SPR013923021 (SPR)s10853-017-1151-1-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Döhler, Franziska verfasserin aut Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. The resulting coefficients of thermal expansion fit well to that of $ Al_{2} %$ O_{3} $. Al2O3 (dpeaa)DE-He213 MgAl2O4 (dpeaa)DE-He213 Glass Powder (dpeaa)DE-He213 Inverse Pole Figure (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Zscheckel, Tilman verfasserin aut Kasch, Susanne verfasserin aut Schmidt, Thomas verfasserin aut Rüssel, Christian verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 16 vom: 04. Mai, Seite 9344-9354 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:16 day:04 month:05 pages:9344-9354 https://dx.doi.org/10.1007/s10853-017-1151-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_206 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 51.00 ASE AR 52 2017 16 04 05 9344-9354 |
spelling |
10.1007/s10853-017-1151-1 doi (DE-627)SPR013923021 (SPR)s10853-017-1151-1-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Döhler, Franziska verfasserin aut Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. The resulting coefficients of thermal expansion fit well to that of $ Al_{2} %$ O_{3} $. Al2O3 (dpeaa)DE-He213 MgAl2O4 (dpeaa)DE-He213 Glass Powder (dpeaa)DE-He213 Inverse Pole Figure (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Zscheckel, Tilman verfasserin aut Kasch, Susanne verfasserin aut Schmidt, Thomas verfasserin aut Rüssel, Christian verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 16 vom: 04. Mai, Seite 9344-9354 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:16 day:04 month:05 pages:9344-9354 https://dx.doi.org/10.1007/s10853-017-1151-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_206 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 51.00 ASE AR 52 2017 16 04 05 9344-9354 |
allfields_unstemmed |
10.1007/s10853-017-1151-1 doi (DE-627)SPR013923021 (SPR)s10853-017-1151-1-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Döhler, Franziska verfasserin aut Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. The resulting coefficients of thermal expansion fit well to that of $ Al_{2} %$ O_{3} $. Al2O3 (dpeaa)DE-He213 MgAl2O4 (dpeaa)DE-He213 Glass Powder (dpeaa)DE-He213 Inverse Pole Figure (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Zscheckel, Tilman verfasserin aut Kasch, Susanne verfasserin aut Schmidt, Thomas verfasserin aut Rüssel, Christian verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 16 vom: 04. Mai, Seite 9344-9354 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:16 day:04 month:05 pages:9344-9354 https://dx.doi.org/10.1007/s10853-017-1151-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_206 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 51.00 ASE AR 52 2017 16 04 05 9344-9354 |
allfieldsGer |
10.1007/s10853-017-1151-1 doi (DE-627)SPR013923021 (SPR)s10853-017-1151-1-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Döhler, Franziska verfasserin aut Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. The resulting coefficients of thermal expansion fit well to that of $ Al_{2} %$ O_{3} $. Al2O3 (dpeaa)DE-He213 MgAl2O4 (dpeaa)DE-He213 Glass Powder (dpeaa)DE-He213 Inverse Pole Figure (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Zscheckel, Tilman verfasserin aut Kasch, Susanne verfasserin aut Schmidt, Thomas verfasserin aut Rüssel, Christian verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 16 vom: 04. Mai, Seite 9344-9354 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:16 day:04 month:05 pages:9344-9354 https://dx.doi.org/10.1007/s10853-017-1151-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_206 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 51.00 ASE AR 52 2017 16 04 05 9344-9354 |
allfieldsSound |
10.1007/s10853-017-1151-1 doi (DE-627)SPR013923021 (SPR)s10853-017-1151-1-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Döhler, Franziska verfasserin aut Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. The resulting coefficients of thermal expansion fit well to that of $ Al_{2} %$ O_{3} $. Al2O3 (dpeaa)DE-He213 MgAl2O4 (dpeaa)DE-He213 Glass Powder (dpeaa)DE-He213 Inverse Pole Figure (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Zscheckel, Tilman verfasserin aut Kasch, Susanne verfasserin aut Schmidt, Thomas verfasserin aut Rüssel, Christian verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 16 vom: 04. Mai, Seite 9344-9354 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:16 day:04 month:05 pages:9344-9354 https://dx.doi.org/10.1007/s10853-017-1151-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_206 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 51.00 ASE AR 52 2017 16 04 05 9344-9354 |
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Enthalten in Journal of materials science 52(2017), 16 vom: 04. Mai, Seite 9344-9354 volume:52 year:2017 number:16 day:04 month:05 pages:9344-9354 |
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Enthalten in Journal of materials science 52(2017), 16 vom: 04. Mai, Seite 9344-9354 volume:52 year:2017 number:16 day:04 month:05 pages:9344-9354 |
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Al2O3 MgAl2O4 Glass Powder Inverse Pole Figure ZnAl2O4 |
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Döhler, Franziska @@aut@@ Zscheckel, Tilman @@aut@@ Kasch, Susanne @@aut@@ Schmidt, Thomas @@aut@@ Rüssel, Christian @@aut@@ |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR013923021</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111004159.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2017 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10853-017-1151-1</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR013923021</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10853-017-1151-1-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">670</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">51.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Döhler, Franziska</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2017</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. 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Mai, Seite 9344-9354</subfield><subfield code="w">(DE-627)315293969</subfield><subfield code="w">(DE-600)2015305-3</subfield><subfield code="x">1573-4803</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:52</subfield><subfield code="g">year:2017</subfield><subfield code="g">number:16</subfield><subfield code="g">day:04</subfield><subfield code="g">month:05</subfield><subfield code="g">pages:9344-9354</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/s10853-017-1151-1</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_SPRINGER</subfield></datafield><datafield 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|
author |
Döhler, Franziska |
spellingShingle |
Döhler, Franziska ddc 670 bkl 51.00 misc Al2O3 misc MgAl2O4 misc Glass Powder misc Inverse Pole Figure misc ZnAl2O4 Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass |
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Döhler, Franziska |
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670 - Manufacturing |
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1573-4803 |
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670 ASE 51.00 bkl Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass Al2O3 (dpeaa)DE-He213 MgAl2O4 (dpeaa)DE-He213 Glass Powder (dpeaa)DE-He213 Inverse Pole Figure (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 |
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ddc 670 bkl 51.00 misc Al2O3 misc MgAl2O4 misc Glass Powder misc Inverse Pole Figure misc ZnAl2O4 |
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ddc 670 bkl 51.00 misc Al2O3 misc MgAl2O4 misc Glass Powder misc Inverse Pole Figure misc ZnAl2O4 |
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ddc 670 bkl 51.00 misc Al2O3 misc MgAl2O4 misc Glass Powder misc Inverse Pole Figure misc ZnAl2O4 |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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title |
Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass |
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(DE-627)SPR013923021 (SPR)s10853-017-1151-1-e |
title_full |
Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass |
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Döhler, Franziska |
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Döhler, Franziska Zscheckel, Tilman Kasch, Susanne Schmidt, Thomas Rüssel, Christian |
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Elektronische Aufsätze |
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Döhler, Franziska |
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10.1007/s10853-017-1151-1 |
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670 |
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verfasserin |
title_sort |
phase formation and microstructure during laser sintering and crystallization of a 4.2 mgo·5.0 zno·44.1 cao·26.7 $ al_{2} %$ o_{3} $·20.0 $ sio_{2} $ glass |
title_auth |
Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass |
abstract |
Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. The resulting coefficients of thermal expansion fit well to that of $ Al_{2} %$ O_{3} $. |
abstractGer |
Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. The resulting coefficients of thermal expansion fit well to that of $ Al_{2} %$ O_{3} $. |
abstract_unstemmed |
Abstract In order to produce housings for high-temperature applications, alumina is a highly advantageous material because it has a high chemical durability and withstands high temperatures. If alumina is to be sealed, materials are necessary which have an adapted coefficient of thermal expansion (8.6 × $ 10^{−6} $ $ K^{−1} $). If temperature-sensitive components have to be encapsulated, a rapid laser sealing process is highly advantageous. This process requires a glass which can rapidly be crystallized. In this paper, a glass powder with the composition 4.2 MgO·5.0 ZnO·44.1·CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ was sintered and subsequently crystallized using a $ CO_{2} $-laser. As crystalline phases, predominantly a solid solution of akermanite and gehlenite (AGSS) was formed and as phases with minor concentrations $ Al_{2} %$ O_{3} $, spinel/gahnite solid solution and ZnO. The AGSS grains have sizes of approximately 5 µm, and Mg and Zn are enriched at the grain boundaries. After sealing at temperatures of 985 and 1135 °C, a similar microstructure and similar grain sizes were observed. The AGSS seems to nucleate at the glass/$ Al_{2} %$ O_{3} $ interface but also in the bulk. The AGSS and all other phases do not show a preferred orientation. The resulting coefficients of thermal expansion fit well to that of $ Al_{2} %$ O_{3} $. |
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container_issue |
16 |
title_short |
Phase formation and microstructure during laser sintering and crystallization of a 4.2 MgO·5.0 ZnO·44.1 CaO·26.7 $ Al_{2} %$ O_{3} $·20.0 $ SiO_{2} $ glass |
url |
https://dx.doi.org/10.1007/s10853-017-1151-1 |
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|
score |
7.3985834 |