Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P
Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Miettinen, Jyrki [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: |
© ASM International 2016 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of phase equilibria and diffusion - Boston, Mass. : Springer, 2004, 37(2016), 5 vom: 31. Mai, Seite 540-547 |
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| Übergeordnetes Werk: |
volume:37 ; year:2016 ; number:5 ; day:31 ; month:05 ; pages:540-547 |
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| DOI / URN: |
10.1007/s11669-016-0472-0 |
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| Katalog-ID: |
SPR02169849X |
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| 520 | |a Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. The correlation between the calculated and the experimental thermodynamic and phase equilibrium data is reasonably good. | ||
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| 650 | 4 | |a thermodynamic modelling |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Vassilev-Urumov, Gueorgui |4 aut | |
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10.1007/s11669-016-0472-0 doi (DE-627)SPR02169849X (SPR)s11669-016-0472-0-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2016 Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. The correlation between the calculated and the experimental thermodynamic and phase equilibrium data is reasonably good. Fe-based systems (dpeaa)DE-He213 Fe-Si-P system (dpeaa)DE-He213 Fe-X-P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 Vassilev-Urumov, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 37(2016), 5 vom: 31. Mai, Seite 540-547 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:37 year:2016 number:5 day:31 month:05 pages:540-547 https://dx.doi.org/10.1007/s11669-016-0472-0 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_101 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_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_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 37 2016 5 31 05 540-547 |
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10.1007/s11669-016-0472-0 doi (DE-627)SPR02169849X (SPR)s11669-016-0472-0-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2016 Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. The correlation between the calculated and the experimental thermodynamic and phase equilibrium data is reasonably good. Fe-based systems (dpeaa)DE-He213 Fe-Si-P system (dpeaa)DE-He213 Fe-X-P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 Vassilev-Urumov, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 37(2016), 5 vom: 31. Mai, Seite 540-547 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:37 year:2016 number:5 day:31 month:05 pages:540-547 https://dx.doi.org/10.1007/s11669-016-0472-0 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_101 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_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_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 37 2016 5 31 05 540-547 |
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10.1007/s11669-016-0472-0 doi (DE-627)SPR02169849X (SPR)s11669-016-0472-0-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2016 Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. The correlation between the calculated and the experimental thermodynamic and phase equilibrium data is reasonably good. Fe-based systems (dpeaa)DE-He213 Fe-Si-P system (dpeaa)DE-He213 Fe-X-P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 Vassilev-Urumov, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 37(2016), 5 vom: 31. Mai, Seite 540-547 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:37 year:2016 number:5 day:31 month:05 pages:540-547 https://dx.doi.org/10.1007/s11669-016-0472-0 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_101 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_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_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 37 2016 5 31 05 540-547 |
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10.1007/s11669-016-0472-0 doi (DE-627)SPR02169849X (SPR)s11669-016-0472-0-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2016 Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. The correlation between the calculated and the experimental thermodynamic and phase equilibrium data is reasonably good. Fe-based systems (dpeaa)DE-He213 Fe-Si-P system (dpeaa)DE-He213 Fe-X-P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 Vassilev-Urumov, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 37(2016), 5 vom: 31. Mai, Seite 540-547 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:37 year:2016 number:5 day:31 month:05 pages:540-547 https://dx.doi.org/10.1007/s11669-016-0472-0 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_101 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_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_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 37 2016 5 31 05 540-547 |
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10.1007/s11669-016-0472-0 doi (DE-627)SPR02169849X (SPR)s11669-016-0472-0-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2016 Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. The correlation between the calculated and the experimental thermodynamic and phase equilibrium data is reasonably good. Fe-based systems (dpeaa)DE-He213 Fe-Si-P system (dpeaa)DE-He213 Fe-X-P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 Vassilev-Urumov, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 37(2016), 5 vom: 31. Mai, Seite 540-547 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:37 year:2016 number:5 day:31 month:05 pages:540-547 https://dx.doi.org/10.1007/s11669-016-0472-0 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_101 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_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_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 37 2016 5 31 05 540-547 |
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Enthalten in Journal of phase equilibria and diffusion 37(2016), 5 vom: 31. Mai, Seite 540-547 volume:37 year:2016 number:5 day:31 month:05 pages:540-547 |
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Enthalten in Journal of phase equilibria and diffusion 37(2016), 5 vom: 31. Mai, Seite 540-547 volume:37 year:2016 number:5 day:31 month:05 pages:540-547 |
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Miettinen, Jyrki @@aut@@ Vassilev-Urumov, Gueorgui @@aut@@ |
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Part 8: Fe-Si-P</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">© ASM International 2016</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. 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| author |
Miettinen, Jyrki |
| spellingShingle |
Miettinen, Jyrki misc Fe-based systems misc Fe-Si-P system misc Fe-X-P database misc phase diagrams misc thermodynamic database misc thermodynamic modelling Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P |
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Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P Fe-based systems (dpeaa)DE-He213 Fe-Si-P system (dpeaa)DE-He213 Fe-X-P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 |
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misc Fe-based systems misc Fe-Si-P system misc Fe-X-P database misc phase diagrams misc thermodynamic database misc thermodynamic modelling |
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misc Fe-based systems misc Fe-Si-P system misc Fe-X-P database misc phase diagrams misc thermodynamic database misc thermodynamic modelling |
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Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P |
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Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P |
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Miettinen, Jyrki |
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Journal of phase equilibria and diffusion |
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Miettinen, Jyrki Vassilev-Urumov, Gueorgui |
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Miettinen, Jyrki |
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10.1007/s11669-016-0472-0 |
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thermodynamic description of ternary fe-x-p systems. part 8: fe-si-p |
| title_auth |
Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P |
| abstract |
Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. The correlation between the calculated and the experimental thermodynamic and phase equilibrium data is reasonably good. © ASM International 2016 |
| abstractGer |
Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. The correlation between the calculated and the experimental thermodynamic and phase equilibrium data is reasonably good. © ASM International 2016 |
| abstract_unstemmed |
Abstract Thermodynamic descriptions of the Fe-Si-P system is developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Si, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-Si, Fe-P and Si-P, are taken from the earlier assessments and those of the Fe-Si-P system are optimized in this study using the experimental thermodynamic and phase equilibrium data of the literature. The solution phases of the system (bcc_A2, fcc_A1, dia_A4, liquid) are described with the substitutional solution model. The compounds are treated either with the sublattice model ($ FeSi_{2} $-H, $ Fe_{2} $P and FeP) either as stoichiometric phases ($ Fe_{3} $P, $ Fe_{2} $Si, $ Fe_{5} %$ Si_{3} $, FeSi, $ FeSi_{2} $-L, SiP, $ SiP_{2} $ and $ FeSi_{4} %$ P_{4} $). No solubility of Fe neither Si in the white P-phase has been modeled. The correlation between the calculated and the experimental thermodynamic and phase equilibrium data is reasonably good. © ASM International 2016 |
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Thermodynamic Description of Ternary Fe-X-P Systems. Part 8: Fe-Si-P |
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https://dx.doi.org/10.1007/s11669-016-0472-0 |
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Vassilev-Urumov, Gueorgui |
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10.1007/s11669-016-0472-0 |
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2024-07-03T23:58:35.901Z |
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| score |
7.399639 |