Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm
Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibrat...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Liu, Hongquan [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2016 |
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| Schlagwörter: |
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| Anmerkung: |
© The Minerals, Metals & Materials Society and ASM International 2016 |
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| Übergeordnetes Werk: |
Enthalten in: Metallurgical and materials transactions - New York, NY : Springer Sciences & Business Media, 1975, 47(2016), 2 vom: 28. Jan., Seite 1113-1123 |
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| Übergeordnetes Werk: |
volume:47 ; year:2016 ; number:2 ; day:28 ; month:01 ; pages:1113-1123 |
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| DOI / URN: |
10.1007/s11663-016-0596-y |
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| Katalog-ID: |
SPR021461384 |
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| 245 | 1 | 0 | |a Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm |
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| 520 | |a Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. The partitioning of ZnO and $ Al_{2} %$ O_{3} $ between the spinel and liquid phases is also discussed in the paper. | ||
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10.1007/s11663-016-0596-y doi (DE-627)SPR021461384 (SPR)s11663-016-0596-y-e DE-627 ger DE-627 rakwb eng Liu, Hongquan verfasserin aut Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society and ASM International 2016 Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. The partitioning of ZnO and $ Al_{2} %$ O_{3} $ between the spinel and liquid phases is also discussed in the paper. Liquidus Temperature (dpeaa)DE-He213 ZnFe2O4 (dpeaa)DE-He213 Copper Smelting (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Primary Phase Field (dpeaa)DE-He213 Cui, Zhixiang aut Chen, Mao aut Zhao, Baojun aut Enthalten in Metallurgical and materials transactions New York, NY : Springer Sciences & Business Media, 1975 47(2016), 2 vom: 28. Jan., Seite 1113-1123 (DE-627)325572062 (DE-600)2037524-4 1543-1916 nnns volume:47 year:2016 number:2 day:28 month:01 pages:1113-1123 https://dx.doi.org/10.1007/s11663-016-0596-y lizenzpflichtig 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_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_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 AR 47 2016 2 28 01 1113-1123 |
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10.1007/s11663-016-0596-y doi (DE-627)SPR021461384 (SPR)s11663-016-0596-y-e DE-627 ger DE-627 rakwb eng Liu, Hongquan verfasserin aut Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society and ASM International 2016 Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. The partitioning of ZnO and $ Al_{2} %$ O_{3} $ between the spinel and liquid phases is also discussed in the paper. Liquidus Temperature (dpeaa)DE-He213 ZnFe2O4 (dpeaa)DE-He213 Copper Smelting (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Primary Phase Field (dpeaa)DE-He213 Cui, Zhixiang aut Chen, Mao aut Zhao, Baojun aut Enthalten in Metallurgical and materials transactions New York, NY : Springer Sciences & Business Media, 1975 47(2016), 2 vom: 28. Jan., Seite 1113-1123 (DE-627)325572062 (DE-600)2037524-4 1543-1916 nnns volume:47 year:2016 number:2 day:28 month:01 pages:1113-1123 https://dx.doi.org/10.1007/s11663-016-0596-y lizenzpflichtig 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_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_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 AR 47 2016 2 28 01 1113-1123 |
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10.1007/s11663-016-0596-y doi (DE-627)SPR021461384 (SPR)s11663-016-0596-y-e DE-627 ger DE-627 rakwb eng Liu, Hongquan verfasserin aut Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society and ASM International 2016 Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. The partitioning of ZnO and $ Al_{2} %$ O_{3} $ between the spinel and liquid phases is also discussed in the paper. Liquidus Temperature (dpeaa)DE-He213 ZnFe2O4 (dpeaa)DE-He213 Copper Smelting (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Primary Phase Field (dpeaa)DE-He213 Cui, Zhixiang aut Chen, Mao aut Zhao, Baojun aut Enthalten in Metallurgical and materials transactions New York, NY : Springer Sciences & Business Media, 1975 47(2016), 2 vom: 28. Jan., Seite 1113-1123 (DE-627)325572062 (DE-600)2037524-4 1543-1916 nnns volume:47 year:2016 number:2 day:28 month:01 pages:1113-1123 https://dx.doi.org/10.1007/s11663-016-0596-y lizenzpflichtig 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_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_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 AR 47 2016 2 28 01 1113-1123 |
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10.1007/s11663-016-0596-y doi (DE-627)SPR021461384 (SPR)s11663-016-0596-y-e DE-627 ger DE-627 rakwb eng Liu, Hongquan verfasserin aut Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society and ASM International 2016 Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. The partitioning of ZnO and $ Al_{2} %$ O_{3} $ between the spinel and liquid phases is also discussed in the paper. Liquidus Temperature (dpeaa)DE-He213 ZnFe2O4 (dpeaa)DE-He213 Copper Smelting (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Primary Phase Field (dpeaa)DE-He213 Cui, Zhixiang aut Chen, Mao aut Zhao, Baojun aut Enthalten in Metallurgical and materials transactions New York, NY : Springer Sciences & Business Media, 1975 47(2016), 2 vom: 28. Jan., Seite 1113-1123 (DE-627)325572062 (DE-600)2037524-4 1543-1916 nnns volume:47 year:2016 number:2 day:28 month:01 pages:1113-1123 https://dx.doi.org/10.1007/s11663-016-0596-y lizenzpflichtig 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_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_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 AR 47 2016 2 28 01 1113-1123 |
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10.1007/s11663-016-0596-y doi (DE-627)SPR021461384 (SPR)s11663-016-0596-y-e DE-627 ger DE-627 rakwb eng Liu, Hongquan verfasserin aut Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society and ASM International 2016 Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. The partitioning of ZnO and $ Al_{2} %$ O_{3} $ between the spinel and liquid phases is also discussed in the paper. Liquidus Temperature (dpeaa)DE-He213 ZnFe2O4 (dpeaa)DE-He213 Copper Smelting (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Primary Phase Field (dpeaa)DE-He213 Cui, Zhixiang aut Chen, Mao aut Zhao, Baojun aut Enthalten in Metallurgical and materials transactions New York, NY : Springer Sciences & Business Media, 1975 47(2016), 2 vom: 28. Jan., Seite 1113-1123 (DE-627)325572062 (DE-600)2037524-4 1543-1916 nnns volume:47 year:2016 number:2 day:28 month:01 pages:1113-1123 https://dx.doi.org/10.1007/s11663-016-0596-y lizenzpflichtig 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_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_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 AR 47 2016 2 28 01 1113-1123 |
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Enthalten in Metallurgical and materials transactions 47(2016), 2 vom: 28. Jan., Seite 1113-1123 volume:47 year:2016 number:2 day:28 month:01 pages:1113-1123 |
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Liquidus Temperature ZnFe2O4 Copper Smelting ZnAl2O4 Primary Phase Field |
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Liu, Hongquan @@aut@@ Cui, Zhixiang @@aut@@ Chen, Mao @@aut@@ Zhao, Baojun @@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">SPR021461384</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230519191134.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2016 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11663-016-0596-y</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR021461384</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s11663-016-0596-y-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="100" ind1="1" ind2=" "><subfield code="a">Liu, Hongquan</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2016</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="500" ind1=" " ind2=" "><subfield code="a">© The Minerals, Metals & Materials Society and ASM International 2016</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. 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Liu, Hongquan |
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Liu, Hongquan misc Liquidus Temperature misc ZnFe2O4 misc Copper Smelting misc ZnAl2O4 misc Primary Phase Field Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm |
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Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm Liquidus Temperature (dpeaa)DE-He213 ZnFe2O4 (dpeaa)DE-He213 Copper Smelting (dpeaa)DE-He213 ZnAl2O4 (dpeaa)DE-He213 Primary Phase Field (dpeaa)DE-He213 |
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Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm |
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Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm |
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phase equilibria study of the zno-“feo”-$ sio_{2} $-$ al_{2} %$ o_{3} $ system at $ po_{2} $ $ 10^{−8} $ atm |
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Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm |
| abstract |
Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. The partitioning of ZnO and $ Al_{2} %$ O_{3} $ between the spinel and liquid phases is also discussed in the paper. © The Minerals, Metals & Materials Society and ASM International 2016 |
| abstractGer |
Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. The partitioning of ZnO and $ Al_{2} %$ O_{3} $ between the spinel and liquid phases is also discussed in the paper. © The Minerals, Metals & Materials Society and ASM International 2016 |
| abstract_unstemmed |
Abstract Phase equilibria studies on ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ system have been carried out in the temperature range between 1523 K and 1573 K (1250 °C and 1300 °C) at $ Po_{2} $ $ 10^{−8} $ atm. Experimental techniques applied in the present study include high temperature equilibration, quenching, and electron probe X-ray microanalysis (EPMA). The compositions of the phases present in the quenched samples were measured by EPMA and used to construct phase diagrams of the pseudo-ternary sections at fixed $ Al_{2} %$ O_{3} $ content. The experimental results show that, spinel, $ SiO_{2} $, and willemite are the major primary phase fields in the composition range investigated. With 2 wt pct $ Al_{2} %$ O_{3} $ content in the liquid phase, the liquidus temperature can be increased by 35 K in the spinel primary phase in comparison with $ Al_{2} %$ O_{3} $-free system. The partitioning of ZnO and $ Al_{2} %$ O_{3} $ between the spinel and liquid phases is also discussed in the paper. © The Minerals, Metals & Materials Society and ASM International 2016 |
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2 |
| title_short |
Phase Equilibria Study of the ZnO-“FeO”-$ SiO_{2} $-$ Al_{2} %$ O_{3} $ System at $ Po_{2} $ $ 10^{−8} $ atm |
| url |
https://dx.doi.org/10.1007/s11663-016-0596-y |
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true |
| author2 |
Cui, Zhixiang Chen, Mao Zhao, Baojun |
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Cui, Zhixiang Chen, Mao Zhao, Baojun |
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| doi_str |
10.1007/s11663-016-0596-y |
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2024-07-03T22:42:07.737Z |
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| score |
7.399907 |