Critical thermodynamic evaluation of oxide systems relevant to fuel ashes and slags, Part 4: Sodium oxide–potassium oxide–silica
Introduction
In continuation of our previous works, [1], [2], [3] the present work is dedicated to the critical thermodynamic evaluation of the ternary system containing potassium, sodium and silicon oxide. This system is important for technical materials, e.g. slags and glasses, and common silicate minerals occurring in rocks. An almost complete phase diagram of the ternary system K2O–Na2O–SiO2 was proposed by Kracek as early as 1932 [4], and it still remains in the focus of attention. Recently, the mixed alkali silicates and a novel single layer silicate have been studied using modern spectroscopic techniques [5], [6]. Because of the experimental difficulties due to the volatility and hygroscopicity of the alkalis, the model approach can be useful for the description of the thermodynamic properties in the available systems. CALPHAD type modelling now permits to treat the phase equilibria and the thermodynamic properties of the complex system.
The binary systems Me2O–SiO2 (Me=Na, K) have been thermodynamically evaluated previously [1] and the new database has been successfully applied for the representation of phase relations and activity data. The liquid phase was described using the modified associate species model [7], [8], which was considered as the most appropriate owing to the fact that it allows an adequate representation of the thermodynamic properties as well as the phase equilibria and can comparatively easily be adjusted to the needs of the respective systems.
The aim of the present work was the generation of a databank extended to the ternary system K2O–Na2O–SiO2. The ternary liquid is described using the above mentioned modified associate species model. The Gibbs energy parameters of the ternary liquid have been determined by optimisation on the basis of available ternary experimental phase relationships. The binary solution data, which were obtained earlier [1], remained unmodified in order to keep consistency of the complete databank.
Section snippets
Phase diagram data
The phase relations in the ternary system K2O–Na2O–SiO2 were studied by Kracek [4] using the quenching method for the determination of liquidus points. The author has only considered the region of the phase diagram from 0 to 50 mole% of the alkali oxides. The binary compounds K2SiO3, Na2SiO3, K2Si2O5, Na2Si2O5, K2Si4O9 and crystalline modifications of silica quartz, tridymite, cristobalite were included. There are no ternary compounds in the system.
Kracek considered the full ternary in terms of
Assessment of Gibbs energy parameters
The Gibbs energy of the liquid phase in the Na2O–K2O–SiO2 system is represented by the modified associate species model [8]. Since there are no ternary compounds in the system, the ternary liquid is represented by a solution containing only the pure component liquids and binary constituents. These are the pure liquid potassium, sodium and silicon oxide and also the binary associate species Na4SiO4⋅2/5, Na2SiO3⋅2/3, Na2Si2O5⋅1/2, K2SiO3⋅2/3, K2Si2O5⋅1/2 and K2Si4O9⋅1/3 which have been applied
Results and discussions
The solution data for the liquid described using the modified associate species model [8] is given in Table 1a. These data concern the interaction parameters which were introduced for the ternary system. The remaining parameters, which relate to the binary sub-systems Me2O–SiO2 (Me=Na, K) were published earlier [1].
The calculated isotherms of the liquidus surfaces in the ternary system Na2O–K2O–SiO2 are given in Fig. 1b and compared with the experimental phase diagram (Fig. 1a) studied by
Conclusions
In the present work the modified associate species model was successfully applied to represent the phase relations in the ternary system Na2O–K2O–SiO2. The Gibbs energy data for the liquid phase were generated for this ternary system by the addition of interaction parameters between the constituents already existing in the liquids of the binary sub-systems. The interaction parameters for the binary systems obtained earlier were kept without change. This is necessary for the development of a
Acknowledgements
This work is part of two projects supported by Bundesministerium für Wirtschaft und Technologie (FKZs 0326844E/9 and 0326885). The authors are grateful to Dr. Ted Besmann, Oak Ridge National Laboratory, and Prof. K. Spear, Pennsylvania State University, for the kind provision of their database.
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