3 research outputs found

    Physicochemical Properties of the (LiF + CaF<sub>2</sub>)<sub>eut</sub> + LaF<sub>3</sub> System: Phase Equilibria, Volume Properties, Electrical Conductivity, and Surface Tension

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    The physicochemical behavior of the molten system (LiF (1) + CaF<sub>2</sub> (2))<sub>eut</sub> + LaF<sub>3</sub> (3) has been studied and the phase equilibria, density and volume properties, electrical conductivity, and surface tension have been selected for investigation. Well-established methods for determination of these physicochemical properties of molten salts have been used, such as thermal analysis, the Archimedean method of hydrostatic weighing, and the phase shift and maximum bubble pressure methods. A significant change in all investigated properties was detected in the region of <i>x</i><sub>3</sub> = 0.04–0.06. In regard to phase equilibria, this region is close to and may contain the eutectic point; in volumetric properties, the initial volume contraction (on increasing mol %) starts to reverse. A sharp change of electrical conductivity reflects the changes in ionic composition, and surface tension also shows different behavior below and above this region

    Physicochemical Properties of the (LiF + CaF<sub>2</sub>)<sub>eut</sub> + LaF<sub>3</sub> System: Phase Equilibria, Volume Properties, Electrical Conductivity, and Surface Tension

    No full text
    The physicochemical behavior of the molten system (LiF (1) + CaF<sub>2</sub> (2))<sub>eut</sub> + LaF<sub>3</sub> (3) has been studied and the phase equilibria, density and volume properties, electrical conductivity, and surface tension have been selected for investigation. Well-established methods for determination of these physicochemical properties of molten salts have been used, such as thermal analysis, the Archimedean method of hydrostatic weighing, and the phase shift and maximum bubble pressure methods. A significant change in all investigated properties was detected in the region of <i>x</i><sub>3</sub> = 0.04–0.06. In regard to phase equilibria, this region is close to and may contain the eutectic point; in volumetric properties, the initial volume contraction (on increasing mol %) starts to reverse. A sharp change of electrical conductivity reflects the changes in ionic composition, and surface tension also shows different behavior below and above this region

    (Oxo)(Fluoro)–Aluminates in KF–Al<sub>2</sub>O<sub>3</sub> System: Thermal Stability and Structural Correlation

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    Precise investigation of part of the phase diagram of KF–Al<sub>2</sub>O<sub>3</sub> system was performed in an experiment combining different techniques. Solidified mixtures of KF–Al<sub>2</sub>O<sub>3</sub> were studied by X-ray powder diffraction and high-field solid-state NMR spectroscopy over a wide range of compositions. To help with the interpretation of the NMR spectra of the solidified samples found as complex admixtures, we synthesized the following pure compounds: KAlO<sub>2</sub>, K<sub>2</sub>Al<sub>22</sub>O<sub>34</sub>, α-K<sub>3</sub>AlF<sub>6</sub>, KAlF<sub>4</sub>, and K<sub>2</sub>Al<sub>2</sub>O<sub>3</sub>F<sub>2</sub>. These compounds were then characterized using various solid-state NMR techniques, including MQ-MAS and D-HMQC. NMR parameters of the pure compounds were finally determined using first-principles density functional theory calculations. The phase diagram of KF–Al<sub>2</sub>O<sub>3</sub> with the alumina content up to 30 mol % was determined by means of thermal analysis. Thermal analysis was also used for the description of the thermal stability of one synthesized compound, K<sub>2</sub>Al<sub>2</sub>O<sub>3</sub>F<sub>2</sub>
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