Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P
Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and thos...
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| Autor*in: |
Miettinen, Jyrki [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2014 |
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| Schlagwörter: |
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| Anmerkung: |
© ASM International 2014 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of phase equilibria and diffusion - Boston, Mass. : Springer, 2004, 36(2014), 1 vom: 18. Okt., Seite 68-77 |
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| Übergeordnetes Werk: |
volume:36 ; year:2014 ; number:1 ; day:18 ; month:10 ; pages:68-77 |
| Links: |
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| DOI / URN: |
10.1007/s11669-014-0351-5 |
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| Katalog-ID: |
SPR021697116 |
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| 100 | 1 | |a Miettinen, Jyrki |e verfasserin |4 aut | |
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| 520 | |a Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. The assessment of this system needs improvement but more experimental information has to be available. | ||
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| 650 | 4 | |a Fe-Nb-P system |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Fe- |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a -P database |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a phase diagrams |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a phosphorous steels |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a thermodynamic modelling |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a thermodynamic database |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Vassilev, Gueorgui |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Journal of phase equilibria and diffusion |d Boston, Mass. : Springer, 2004 |g 36(2014), 1 vom: 18. Okt., Seite 68-77 |w (DE-627)626050863 |w (DE-600)2552809-9 |x 1863-7345 |7 nnns |
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10.1007/s11669-014-0351-5 doi (DE-627)SPR021697116 (SPR)s11669-014-0351-5-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2014 Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. The assessment of this system needs improvement but more experimental information has to be available. Fe-based systems (dpeaa)DE-He213 Fe-Nb-P system (dpeaa)DE-He213 Fe- (dpeaa)DE-He213 -P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 phosphorous steels (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 Vassilev, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 36(2014), 1 vom: 18. Okt., Seite 68-77 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:36 year:2014 number:1 day:18 month:10 pages:68-77 https://dx.doi.org/10.1007/s11669-014-0351-5 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 36 2014 1 18 10 68-77 |
| spelling |
10.1007/s11669-014-0351-5 doi (DE-627)SPR021697116 (SPR)s11669-014-0351-5-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2014 Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. The assessment of this system needs improvement but more experimental information has to be available. Fe-based systems (dpeaa)DE-He213 Fe-Nb-P system (dpeaa)DE-He213 Fe- (dpeaa)DE-He213 -P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 phosphorous steels (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 Vassilev, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 36(2014), 1 vom: 18. Okt., Seite 68-77 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:36 year:2014 number:1 day:18 month:10 pages:68-77 https://dx.doi.org/10.1007/s11669-014-0351-5 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 36 2014 1 18 10 68-77 |
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10.1007/s11669-014-0351-5 doi (DE-627)SPR021697116 (SPR)s11669-014-0351-5-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2014 Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. The assessment of this system needs improvement but more experimental information has to be available. Fe-based systems (dpeaa)DE-He213 Fe-Nb-P system (dpeaa)DE-He213 Fe- (dpeaa)DE-He213 -P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 phosphorous steels (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 Vassilev, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 36(2014), 1 vom: 18. Okt., Seite 68-77 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:36 year:2014 number:1 day:18 month:10 pages:68-77 https://dx.doi.org/10.1007/s11669-014-0351-5 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 36 2014 1 18 10 68-77 |
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10.1007/s11669-014-0351-5 doi (DE-627)SPR021697116 (SPR)s11669-014-0351-5-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2014 Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. The assessment of this system needs improvement but more experimental information has to be available. Fe-based systems (dpeaa)DE-He213 Fe-Nb-P system (dpeaa)DE-He213 Fe- (dpeaa)DE-He213 -P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 phosphorous steels (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 Vassilev, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 36(2014), 1 vom: 18. Okt., Seite 68-77 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:36 year:2014 number:1 day:18 month:10 pages:68-77 https://dx.doi.org/10.1007/s11669-014-0351-5 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 36 2014 1 18 10 68-77 |
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10.1007/s11669-014-0351-5 doi (DE-627)SPR021697116 (SPR)s11669-014-0351-5-e DE-627 ger DE-627 rakwb eng Miettinen, Jyrki verfasserin aut Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © ASM International 2014 Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. The assessment of this system needs improvement but more experimental information has to be available. Fe-based systems (dpeaa)DE-He213 Fe-Nb-P system (dpeaa)DE-He213 Fe- (dpeaa)DE-He213 -P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 phosphorous steels (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 Vassilev, Gueorgui aut Enthalten in Journal of phase equilibria and diffusion Boston, Mass. : Springer, 2004 36(2014), 1 vom: 18. Okt., Seite 68-77 (DE-627)626050863 (DE-600)2552809-9 1863-7345 nnns volume:36 year:2014 number:1 day:18 month:10 pages:68-77 https://dx.doi.org/10.1007/s11669-014-0351-5 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 36 2014 1 18 10 68-77 |
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Enthalten in Journal of phase equilibria and diffusion 36(2014), 1 vom: 18. Okt., Seite 68-77 volume:36 year:2014 number:1 day:18 month:10 pages:68-77 |
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Enthalten in Journal of phase equilibria and diffusion 36(2014), 1 vom: 18. Okt., Seite 68-77 volume:36 year:2014 number:1 day:18 month:10 pages:68-77 |
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Miettinen, Jyrki @@aut@@ Vassilev, Gueorgui @@aut@@ |
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Part 5: Fe-Nb-P</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2014</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 2014</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. 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Miettinen, Jyrki |
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Miettinen, Jyrki misc Fe-based systems misc Fe-Nb-P system misc Fe- misc -P database misc phase diagrams misc phosphorous steels misc thermodynamic modelling misc thermodynamic database Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P |
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Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P Fe-based systems (dpeaa)DE-He213 Fe-Nb-P system (dpeaa)DE-He213 Fe- (dpeaa)DE-He213 -P database (dpeaa)DE-He213 phase diagrams (dpeaa)DE-He213 phosphorous steels (dpeaa)DE-He213 thermodynamic modelling (dpeaa)DE-He213 thermodynamic database (dpeaa)DE-He213 |
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thermodynamic description of ternary fe-x-p systems. part 5: fe-nb-p |
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Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P |
| abstract |
Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. The assessment of this system needs improvement but more experimental information has to be available. © ASM International 2014 |
| abstractGer |
Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. The assessment of this system needs improvement but more experimental information has to be available. © ASM International 2014 |
| abstract_unstemmed |
Abstract Thermodynamic descriptions of the Fe-Nb-P system and its binary sub-system, Fe-Nb, are developed in the frame of a new Fe-X-P (X = Al, Cr, Cu, Mn, Mo, Nb, Ni, Si, Ti) database. The thermodynamic parameters of the binary sub-systems, Fe-P and Nb-P, are taken from earlier assessments and those of the Fe-Nb-P and Fe-Nb systems are optimized in this study using literature experimental thermodynamic and phase equilibrium data. The solution phases of the system (i.e. bcc_A2, fcc_A1, Liquid) are described with the substitutional solution model. The phase Mu ($ Fe_{7} %$ Nb_{6} $) has been modeled as (Fe,Nb)7(Nb)6, while $ Fe_{2} $P and FeNbP, have been modeled both as (Fe,Nb)2(P). All other phases ($ Fe_{2} $Nb, $ Fe_{3} $P, FeP, $ Nb_{3} $P, $ Nb_{7} %$ P_{4} $, NbP, $ NbP_{2} $, $ FeNb_{2} $P, $ FeNb_{4} $P, (P)) are treated as stoichiometric. The assessment of this system needs improvement but more experimental information has to be available. © ASM International 2014 |
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| title_short |
Thermodynamic Description of Ternary Fe-X-P systems. Part 5: Fe-Nb-P |
| url |
https://dx.doi.org/10.1007/s11669-014-0351-5 |
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| author2 |
Vassilev, Gueorgui |
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10.1007/s11669-014-0351-5 |
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2024-07-03T23:58:12.052Z |
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| score |
7.399806 |