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
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
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
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>