Role of basicity and tetrahedral speciation in controlling the thermodynamic properties of silicate liquids. I - The system CaO-MgO-Al2O3-SiO2
Activity coefficients of oxide components in the system CaO-MgO-Al2O3-SiO2 (CMAS) were calculated with the model of Berman (1983) and used to explore large-scale relationships among these variables and between them and the liquid composition. On the basis of Berman's model, the natural logarith...
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Published in: | Geochimica et cosmochimica acta Vol. 66; no. 1; pp. 93 - 107 |
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Main Author: | |
Format: | Journal Article |
Language: | English |
Published: |
01-01-2002
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Online Access: | Get full text |
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Summary: | Activity coefficients of oxide components in the system CaO-MgO-Al2O3-SiO2 (CMAS) were calculated with the model of Berman (1983) and used to explore large-scale relationships among these variables and between them and the liquid composition. On the basis of Berman's model, the natural logarithm of the activity coefficient of MgO, ln(gamma MgO)(Liq), and ln(gamma MgO)(Liq /gamma SiO2)(Liq) are nearly linear functions of ln(gamma CaO)(Liq). All three of these variables are simple functions of the optical basicity Lambda with which they display minima near Lambda about 0.54 that are generated by liquids with low ratios of nonbridging to tetrahedral oxygens (NBO/T) ( < 0.3) and a mole fraction ratio, X(SiO2(Liq))/X(Al2O3(Liq)), in the range 4 to 20. Variations in ln(gamma CaO)(Liq) at constant Lambda near the minimum are due mostly to liquids with (X(CaO)(Liq) + X(MgO(Liq)) /X(Al2O3(Liq)) < 1. The correlations with optical basicity imply that the electron donor power is an important factor in determining the thermodynamic properties of aluminosilicate liquids.For a constant NBO/T, ln(gamma CaO(Liq)/gamma Al2O3(Liq)) and ln(gamma MgO(Liq) gamma Al2O3(Liq)) form curves in terms of X(SiO2)(Liq)/X(Al2O3)(Liq). The same liquids that generate minima in the Lambda plots are also associated with minima in ln(gamma CaO(Liq) gamma Al2O3(Liq)) and ln(gamma MgO(Liq) gamma Al2O3(Liq)) as a function of X(SiO2(Liq))/X(Al2O3)(Liq)). In addition, there are maxima or sharp changes in slope for NBO/T > 0.3, which occur for X(SiO2(Liq))/X(Al2O3(Liq)) ranging from about 0 to about 6 and increase with increasing NBO/T. The systematic variations in activity coefficients as a function of composition and optical basicity reflect underlying shifts in speciation as the composition of the liquid is changed. On the basis of correlations among the activity coefficients, it is likely that the use of CaO, an exchange component such as SiMg(-1) and two of MgO, CaAl2O4, or MgAl2O4 would yield significant savings in the number of parameters required to model the excess free energy surface of liquids over large portions of CMAS relative to the use of oxide end members.Systematic behavior of thermodynamic properties extends to small amounts of other elements dissolved in otherwise CMAS liquids. For example, ln X(sub Fe(2+) sup Liq)/X(sub Fe(3+) sup Liq) at constant oxygen fugacity is linearly correlated with ln(gamma CaO(Liq)). Similarly, ln(CS), where CS is the sulfide capacity is linearly correlated at constant temperature with each of the optical basicity, ln(gamma CaO(Liq)) and ln(gamma CaO(Liq)), although the correlation for the latter breaks down for low values of Lambda. The well-known systematic behavior of sulfide capacity as a function of optical basicity for systems inside as well as outside CMAS suggests that ln(gamma CaS(Liq) is also a simple function of optical basicity and that the relationships observed among the activity coefficients in CMAS may hold for more complex systems. (Author) |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 content type line 23 ObjectType-Feature-1 |
ISSN: | 0016-7037 |