Abstract <p>Feldspars of the KGaSi<sub>3</sub>O<sub>8</sub>–RbGaSi<sub>3</sub>O<sub>8</sub> series were synthesized at 550°C and 1.5 kbar, and their exchange reactions with 1 M KCl + 1 M RbCl solution were investigated. Using the experimental data, Margules parameters were calculated for the description of the excess mixing energies of the (K,Rb)GaSi<sub>3</sub>O<sub>8</sub> solid solution: <i>W</i><sup><i>G</i></sup>1 = <i>W</i><sup><i>G</i></sup>2 = 4.46 ± 0.11 kJ/mol. We refined the unit-cell parameters of the solid solutions; the excess mixing volume is described by the Margules model: <i>W</i><sup><i>V</i></sup>1 = 2.647 ± 0.05 and <i>W</i><sup><i>V</i></sup>2 = –0.883 ± 0.04 cm<sup>3</sup>/mol. The results were compared with feldspars studied previously. Empirical relations were proposed for the calculation of the energy Margules model and unit-cell volumes for various minerals with the feldspar structure.</p>

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Experimental Investigation of Cation Exchange Equilibria of the Gallium Feldspar Solid Solution (K, Rb)GaSi3O8 with KCl–RbCl–H2O Fluids at 550°C and 1.5 kbar with Applications to the Description of the Properties of Solid Solutions with the Feldspar Structure

  • A. R. Kotelnikov,
  • N. I. Suk,
  • Z. A. Kotelnikova,
  • G. M. Akhmedzhanova,
  • N. A. Drozhzhina

摘要

Abstract

Feldspars of the KGaSi3O8–RbGaSi3O8 series were synthesized at 550°C and 1.5 kbar, and their exchange reactions with 1 M KCl + 1 M RbCl solution were investigated. Using the experimental data, Margules parameters were calculated for the description of the excess mixing energies of the (K,Rb)GaSi3O8 solid solution: WG1 = WG2 = 4.46 ± 0.11 kJ/mol. We refined the unit-cell parameters of the solid solutions; the excess mixing volume is described by the Margules model: WV1 = 2.647 ± 0.05 and WV2 = –0.883 ± 0.04 cm3/mol. The results were compared with feldspars studied previously. Empirical relations were proposed for the calculation of the energy Margules model and unit-cell volumes for various minerals with the feldspar structure.