Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K
Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidifi...
Ausführliche Beschreibung
Autor*in: |
Mlynáriková, Jarmila [verfasserIn] Boča, Miroslav [verfasserIn] Gurišová, Veronika [verfasserIn] Macková, Iveta [verfasserIn] Netriová, Zuzana [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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Übergeordnetes Werk: |
Enthalten in: Journal of thermal analysis and calorimetry - Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969, 124(2016), 2 vom: 20. Jan., Seite 973-987 |
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Übergeordnetes Werk: |
volume:124 ; year:2016 ; number:2 ; day:20 ; month:01 ; pages:973-987 |
Links: |
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DOI / URN: |
10.1007/s10973-015-5233-5 |
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Katalog-ID: |
SPR015540863 |
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245 | 1 | 0 | |a Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K |
264 | 1 | |c 2016 | |
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520 | |a Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. With increasing temperature, partial molar volumes of $ LnF_{3} $ decrease even to negative values. | ||
650 | 4 | |a Molten salt |7 (dpeaa)DE-He213 | |
650 | 4 | |a Temperature of primary crystallisation |7 (dpeaa)DE-He213 | |
650 | 4 | |a Density |7 (dpeaa)DE-He213 | |
650 | 4 | |a Molar volume |7 (dpeaa)DE-He213 | |
650 | 4 | |a Partial molar volume |7 (dpeaa)DE-He213 | |
650 | 4 | |a Samarium fluoride |7 (dpeaa)DE-He213 | |
650 | 4 | |a Gadolinium fluoride |7 (dpeaa)DE-He213 | |
650 | 4 | |a Neodymium fluoride |7 (dpeaa)DE-He213 | |
650 | 4 | |a Molten salts |7 (dpeaa)DE-He213 | |
700 | 1 | |a Boča, Miroslav |e verfasserin |4 aut | |
700 | 1 | |a Gurišová, Veronika |e verfasserin |4 aut | |
700 | 1 | |a Macková, Iveta |e verfasserin |4 aut | |
700 | 1 | |a Netriová, Zuzana |e verfasserin |4 aut | |
773 | 0 | 8 | |i Enthalten in |t Journal of thermal analysis and calorimetry |d Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 |g 124(2016), 2 vom: 20. Jan., Seite 973-987 |w (DE-627)315295422 |w (DE-600)2017304-0 |x 1572-8943 |7 nnns |
773 | 1 | 8 | |g volume:124 |g year:2016 |g number:2 |g day:20 |g month:01 |g pages:973-987 |
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2016 |
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10.1007/s10973-015-5233-5 doi (DE-627)SPR015540863 (SPR)s10973-015-5233-5-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Mlynáriková, Jarmila verfasserin aut Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. With increasing temperature, partial molar volumes of $ LnF_{3} $ decrease even to negative values. Molten salt (dpeaa)DE-He213 Temperature of primary crystallisation (dpeaa)DE-He213 Density (dpeaa)DE-He213 Molar volume (dpeaa)DE-He213 Partial molar volume (dpeaa)DE-He213 Samarium fluoride (dpeaa)DE-He213 Gadolinium fluoride (dpeaa)DE-He213 Neodymium fluoride (dpeaa)DE-He213 Molten salts (dpeaa)DE-He213 Boča, Miroslav verfasserin aut Gurišová, Veronika verfasserin aut Macková, Iveta verfasserin aut Netriová, Zuzana verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 124(2016), 2 vom: 20. Jan., Seite 973-987 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:124 year:2016 number:2 day:20 month:01 pages:973-987 https://dx.doi.org/10.1007/s10973-015-5233-5 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 124 2016 2 20 01 973-987 |
spelling |
10.1007/s10973-015-5233-5 doi (DE-627)SPR015540863 (SPR)s10973-015-5233-5-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Mlynáriková, Jarmila verfasserin aut Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. With increasing temperature, partial molar volumes of $ LnF_{3} $ decrease even to negative values. Molten salt (dpeaa)DE-He213 Temperature of primary crystallisation (dpeaa)DE-He213 Density (dpeaa)DE-He213 Molar volume (dpeaa)DE-He213 Partial molar volume (dpeaa)DE-He213 Samarium fluoride (dpeaa)DE-He213 Gadolinium fluoride (dpeaa)DE-He213 Neodymium fluoride (dpeaa)DE-He213 Molten salts (dpeaa)DE-He213 Boča, Miroslav verfasserin aut Gurišová, Veronika verfasserin aut Macková, Iveta verfasserin aut Netriová, Zuzana verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 124(2016), 2 vom: 20. Jan., Seite 973-987 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:124 year:2016 number:2 day:20 month:01 pages:973-987 https://dx.doi.org/10.1007/s10973-015-5233-5 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 124 2016 2 20 01 973-987 |
allfields_unstemmed |
10.1007/s10973-015-5233-5 doi (DE-627)SPR015540863 (SPR)s10973-015-5233-5-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Mlynáriková, Jarmila verfasserin aut Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. With increasing temperature, partial molar volumes of $ LnF_{3} $ decrease even to negative values. Molten salt (dpeaa)DE-He213 Temperature of primary crystallisation (dpeaa)DE-He213 Density (dpeaa)DE-He213 Molar volume (dpeaa)DE-He213 Partial molar volume (dpeaa)DE-He213 Samarium fluoride (dpeaa)DE-He213 Gadolinium fluoride (dpeaa)DE-He213 Neodymium fluoride (dpeaa)DE-He213 Molten salts (dpeaa)DE-He213 Boča, Miroslav verfasserin aut Gurišová, Veronika verfasserin aut Macková, Iveta verfasserin aut Netriová, Zuzana verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 124(2016), 2 vom: 20. Jan., Seite 973-987 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:124 year:2016 number:2 day:20 month:01 pages:973-987 https://dx.doi.org/10.1007/s10973-015-5233-5 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 124 2016 2 20 01 973-987 |
allfieldsGer |
10.1007/s10973-015-5233-5 doi (DE-627)SPR015540863 (SPR)s10973-015-5233-5-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Mlynáriková, Jarmila verfasserin aut Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. With increasing temperature, partial molar volumes of $ LnF_{3} $ decrease even to negative values. Molten salt (dpeaa)DE-He213 Temperature of primary crystallisation (dpeaa)DE-He213 Density (dpeaa)DE-He213 Molar volume (dpeaa)DE-He213 Partial molar volume (dpeaa)DE-He213 Samarium fluoride (dpeaa)DE-He213 Gadolinium fluoride (dpeaa)DE-He213 Neodymium fluoride (dpeaa)DE-He213 Molten salts (dpeaa)DE-He213 Boča, Miroslav verfasserin aut Gurišová, Veronika verfasserin aut Macková, Iveta verfasserin aut Netriová, Zuzana verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 124(2016), 2 vom: 20. Jan., Seite 973-987 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:124 year:2016 number:2 day:20 month:01 pages:973-987 https://dx.doi.org/10.1007/s10973-015-5233-5 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 124 2016 2 20 01 973-987 |
allfieldsSound |
10.1007/s10973-015-5233-5 doi (DE-627)SPR015540863 (SPR)s10973-015-5233-5-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Mlynáriková, Jarmila verfasserin aut Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. With increasing temperature, partial molar volumes of $ LnF_{3} $ decrease even to negative values. Molten salt (dpeaa)DE-He213 Temperature of primary crystallisation (dpeaa)DE-He213 Density (dpeaa)DE-He213 Molar volume (dpeaa)DE-He213 Partial molar volume (dpeaa)DE-He213 Samarium fluoride (dpeaa)DE-He213 Gadolinium fluoride (dpeaa)DE-He213 Neodymium fluoride (dpeaa)DE-He213 Molten salts (dpeaa)DE-He213 Boča, Miroslav verfasserin aut Gurišová, Veronika verfasserin aut Macková, Iveta verfasserin aut Netriová, Zuzana verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 124(2016), 2 vom: 20. Jan., Seite 973-987 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:124 year:2016 number:2 day:20 month:01 pages:973-987 https://dx.doi.org/10.1007/s10973-015-5233-5 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 124 2016 2 20 01 973-987 |
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Enthalten in Journal of thermal analysis and calorimetry 124(2016), 2 vom: 20. Jan., Seite 973-987 volume:124 year:2016 number:2 day:20 month:01 pages:973-987 |
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Enthalten in Journal of thermal analysis and calorimetry 124(2016), 2 vom: 20. Jan., Seite 973-987 volume:124 year:2016 number:2 day:20 month:01 pages:973-987 |
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Molten salt Temperature of primary crystallisation Density Molar volume Partial molar volume Samarium fluoride Gadolinium fluoride Neodymium fluoride Molten salts |
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Journal of thermal analysis and calorimetry |
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Mlynáriková, Jarmila @@aut@@ Boča, Miroslav @@aut@@ Gurišová, Veronika @@aut@@ Macková, Iveta @@aut@@ Netriová, Zuzana @@aut@@ |
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2016-01-20T00:00:00Z |
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Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. 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|
author |
Mlynáriková, Jarmila |
spellingShingle |
Mlynáriková, Jarmila ddc 660 bkl 35.00 misc Molten salt misc Temperature of primary crystallisation misc Density misc Molar volume misc Partial molar volume misc Samarium fluoride misc Gadolinium fluoride misc Neodymium fluoride misc Molten salts Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K |
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1572-8943 |
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660 ASE 35.00 bkl Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K Molten salt (dpeaa)DE-He213 Temperature of primary crystallisation (dpeaa)DE-He213 Density (dpeaa)DE-He213 Molar volume (dpeaa)DE-He213 Partial molar volume (dpeaa)DE-He213 Samarium fluoride (dpeaa)DE-He213 Gadolinium fluoride (dpeaa)DE-He213 Neodymium fluoride (dpeaa)DE-He213 Molten salts (dpeaa)DE-He213 |
topic |
ddc 660 bkl 35.00 misc Molten salt misc Temperature of primary crystallisation misc Density misc Molar volume misc Partial molar volume misc Samarium fluoride misc Gadolinium fluoride misc Neodymium fluoride misc Molten salts |
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ddc 660 bkl 35.00 misc Molten salt misc Temperature of primary crystallisation misc Density misc Molar volume misc Partial molar volume misc Samarium fluoride misc Gadolinium fluoride misc Neodymium fluoride misc Molten salts |
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ddc 660 bkl 35.00 misc Molten salt misc Temperature of primary crystallisation misc Density misc Molar volume misc Partial molar volume misc Samarium fluoride misc Gadolinium fluoride misc Neodymium fluoride misc Molten salts |
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title |
Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K |
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Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K |
author_sort |
Mlynáriková, Jarmila |
journal |
Journal of thermal analysis and calorimetry |
journalStr |
Journal of thermal analysis and calorimetry |
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eng |
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600 - Technology |
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marc |
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2016 |
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container_start_page |
973 |
author_browse |
Mlynáriková, Jarmila Boča, Miroslav Gurišová, Veronika Macková, Iveta Netriová, Zuzana |
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124 |
class |
660 ASE 35.00 bkl |
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Elektronische Aufsätze |
author-letter |
Mlynáriková, Jarmila |
doi_str_mv |
10.1007/s10973-015-5233-5 |
dewey-full |
660 |
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verfasserin |
title_sort |
thermal analysis and volume properties of the systems (lif–$ caf_{2} $)eut.–$ lnf_{3} $ (ln = sm, gd, and nd) up to 1273 k |
title_auth |
Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K |
abstract |
Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. With increasing temperature, partial molar volumes of $ LnF_{3} $ decrease even to negative values. |
abstractGer |
Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. With increasing temperature, partial molar volumes of $ LnF_{3} $ decrease even to negative values. |
abstract_unstemmed |
Abstract Systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) were investigated by means of thermal analysis and density measurements. Temperatures of primary crystallisation were measured and solidified samples were analysed by XRD as well as by SEM images and EDX mapping of the solidified samples. Densities of individual melts were measured by hydrostatic weighting (Archimedean method). Consequently, molar volumes were calculated. Unusual behaviour was observed in all three cases, when molar volumes decrease with initial $ LnF_{3} $ additions up to 1 mol % of $ LnF_{3} $. Further $ LnF_{3} $ additions result in molar volumes increase. In the case of $ GdF_{3} $ system, anomalous molar volume behaviour was observed: over 1 mol % of $ GdF_{3} $ molar volume is higher at lower temperatures. Partial molar volumes of $ LnF_{3} $ components were analysed by both simple linear or polynomial regression and multicomponent polynomial regression using least square parameters minimisation procedure. With increasing temperature, partial molar volumes of $ LnF_{3} $ decrease even to negative values. |
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container_issue |
2 |
title_short |
Thermal analysis and volume properties of the systems (LiF–$ CaF_{2} $)eut.–$ LnF_{3} $ (Ln = Sm, Gd, and Nd) up to 1273 K |
url |
https://dx.doi.org/10.1007/s10973-015-5233-5 |
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author2 |
Boča, Miroslav Gurišová, Veronika Macková, Iveta Netriová, Zuzana |
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Boča, Miroslav Gurišová, Veronika Macková, Iveta Netriová, Zuzana |
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up_date |
2024-07-03T16:54:39.031Z |
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score |
7.401434 |