Details
Original language | English |
---|---|
Pages (from-to) | 19-30 |
Number of pages | 12 |
Journal | Journal of non-crystalline solids |
Volume | 390 |
Early online date | 12 Mar 2014 |
Publication status | Published - 15 Apr 2014 |
Abstract
We determined the heat capacities of four series of glasses and liquids of basaltic and basaltic andesite compositions from remelted volcanic rock samples and Fe-free synthetic analogues. The samples are low-alkali, Ca- and Mg-rich aluminosilicates with non-bridging oxygen to tetrahedrally-coordinated cation ratios (NBO/T) ranging between 0.33 and 0.67. Differential scanning calorimetry measurements were performed at atmospheric pressure between room temperature and ∼ 100 K above the glass transition for hydrous samples and up to ∼ 1800 K for dry samples. The water contents investigated range up to 5.34 wt.% (16.4 mol%). Water does not measurably affect the heat capacity of glasses. We derived a new value of the partial molar heat capacity of water in silicate glasses of C̄P,H2Oglass=82.804+10-3T-48.274×10 -5T-2 (J/mol K) using our new data in combination with literature data on more and less polymerized compositions. The increase in heat capacity at the glass transition is of the order of ∼ 30-40% and generally increases with increasing water content. The onset of the glass transition in hydrous samples occurs below the Dulong-Petit limit of 3R/g atom. The configurational heat capacity, i.e., the magnitude of the change in heat capacity observed at the glass transition, generally increases as polymerization decreases and as water content increases. We obtained a partial molar heat capacity of water in silicate liquids of basaltic composition of ∼ 86 J/mol K. This value is comparable to the partial molar values for the major oxides which range from ∼ 79 to 230 J/mol K. The partial molar heat capacity of water in silicate liquids appears to be compositionally-dependent, increasing as melt polymerization decreases. Such a dependence is certainly linked to the speciation and structural roles of water in complex silicate melts, however, a single value of ∼ 93 J/mol K could reproduce the heat capacity of hydrous liquids of a wide range of NBO/T (0-1.51) at temperatures up to ∼ 100 K above the glass transition and water contents of 0-3.76 wt.% with a root-mean square deviation of only 3.23 J/mol K.
Keywords
- Basalt, Glasses, Heat capacity, Melts, Water
ASJC Scopus subject areas
- Materials Science(all)
- Electronic, Optical and Magnetic Materials
- Materials Science(all)
- Ceramics and Composites
- Physics and Astronomy(all)
- Condensed Matter Physics
- Materials Science(all)
- Materials Chemistry
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In: Journal of non-crystalline solids, Vol. 390, 15.04.2014, p. 19-30.
Research output: Contribution to journal › Article › Research › peer review
}
TY - JOUR
T1 - Heat capacity of hydrous basaltic glasses and liquids
AU - Robert, Geneviève
AU - Whittington, Alan G.
AU - Stechern, André
AU - Behrens, Harald
N1 - Funding Information: We thank J. Knipping at Leibniz Universität Hannover (LUH) for KFT analyses, A. Sehlke (MU) and S. Wilke (LUH) for help with IR measurements, and O. Dietrich at LUH for impeccable sample preparation. This research is supported by the NSF via grant EAR-0748411 (AGW). Calorimetry facilities at MU are supported by the NSF via grant EAR-1220051 and by NASA through award PGG-NNX12A044G (AGW). Additional support by the German DFG grant BE 1720/24-1,2 (HB) and DAAD and NSERC fellowships (GR) is acknowledged.
PY - 2014/4/15
Y1 - 2014/4/15
N2 - We determined the heat capacities of four series of glasses and liquids of basaltic and basaltic andesite compositions from remelted volcanic rock samples and Fe-free synthetic analogues. The samples are low-alkali, Ca- and Mg-rich aluminosilicates with non-bridging oxygen to tetrahedrally-coordinated cation ratios (NBO/T) ranging between 0.33 and 0.67. Differential scanning calorimetry measurements were performed at atmospheric pressure between room temperature and ∼ 100 K above the glass transition for hydrous samples and up to ∼ 1800 K for dry samples. The water contents investigated range up to 5.34 wt.% (16.4 mol%). Water does not measurably affect the heat capacity of glasses. We derived a new value of the partial molar heat capacity of water in silicate glasses of C̄P,H2Oglass=82.804+10-3T-48.274×10 -5T-2 (J/mol K) using our new data in combination with literature data on more and less polymerized compositions. The increase in heat capacity at the glass transition is of the order of ∼ 30-40% and generally increases with increasing water content. The onset of the glass transition in hydrous samples occurs below the Dulong-Petit limit of 3R/g atom. The configurational heat capacity, i.e., the magnitude of the change in heat capacity observed at the glass transition, generally increases as polymerization decreases and as water content increases. We obtained a partial molar heat capacity of water in silicate liquids of basaltic composition of ∼ 86 J/mol K. This value is comparable to the partial molar values for the major oxides which range from ∼ 79 to 230 J/mol K. The partial molar heat capacity of water in silicate liquids appears to be compositionally-dependent, increasing as melt polymerization decreases. Such a dependence is certainly linked to the speciation and structural roles of water in complex silicate melts, however, a single value of ∼ 93 J/mol K could reproduce the heat capacity of hydrous liquids of a wide range of NBO/T (0-1.51) at temperatures up to ∼ 100 K above the glass transition and water contents of 0-3.76 wt.% with a root-mean square deviation of only 3.23 J/mol K.
AB - We determined the heat capacities of four series of glasses and liquids of basaltic and basaltic andesite compositions from remelted volcanic rock samples and Fe-free synthetic analogues. The samples are low-alkali, Ca- and Mg-rich aluminosilicates with non-bridging oxygen to tetrahedrally-coordinated cation ratios (NBO/T) ranging between 0.33 and 0.67. Differential scanning calorimetry measurements were performed at atmospheric pressure between room temperature and ∼ 100 K above the glass transition for hydrous samples and up to ∼ 1800 K for dry samples. The water contents investigated range up to 5.34 wt.% (16.4 mol%). Water does not measurably affect the heat capacity of glasses. We derived a new value of the partial molar heat capacity of water in silicate glasses of C̄P,H2Oglass=82.804+10-3T-48.274×10 -5T-2 (J/mol K) using our new data in combination with literature data on more and less polymerized compositions. The increase in heat capacity at the glass transition is of the order of ∼ 30-40% and generally increases with increasing water content. The onset of the glass transition in hydrous samples occurs below the Dulong-Petit limit of 3R/g atom. The configurational heat capacity, i.e., the magnitude of the change in heat capacity observed at the glass transition, generally increases as polymerization decreases and as water content increases. We obtained a partial molar heat capacity of water in silicate liquids of basaltic composition of ∼ 86 J/mol K. This value is comparable to the partial molar values for the major oxides which range from ∼ 79 to 230 J/mol K. The partial molar heat capacity of water in silicate liquids appears to be compositionally-dependent, increasing as melt polymerization decreases. Such a dependence is certainly linked to the speciation and structural roles of water in complex silicate melts, however, a single value of ∼ 93 J/mol K could reproduce the heat capacity of hydrous liquids of a wide range of NBO/T (0-1.51) at temperatures up to ∼ 100 K above the glass transition and water contents of 0-3.76 wt.% with a root-mean square deviation of only 3.23 J/mol K.
KW - Basalt
KW - Glasses
KW - Heat capacity
KW - Melts
KW - Water
UR - http://www.scopus.com/inward/record.url?scp=84896509856&partnerID=8YFLogxK
U2 - 10.1016/j.jnoncrysol.2014.02.011
DO - 10.1016/j.jnoncrysol.2014.02.011
M3 - Article
AN - SCOPUS:84896509856
VL - 390
SP - 19
EP - 30
JO - Journal of non-crystalline solids
JF - Journal of non-crystalline solids
SN - 0022-3093
ER -