Na2SO4–NaCl–H2O system with a binary homogeneous critical point: Phase equilibria at 475–520°C and to 130 MPa
- Authors: Urusova M.A.1, Valyashko V.M.1
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Affiliations:
- Kurnakov Institute of General and Inorganic Chemistry
- Issue: Vol 62, No 6 (2017)
- Pages: 843-853
- Section: Physicochemical Analysis of Inorganic Systems
- URL: https://journals.rcsi.science/0036-0236/article/view/167796
- DOI: https://doi.org/10.1134/S0036023617060250
- ID: 167796
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Abstract
Phase equilibria were studied at temperatures 475–520°C and a pressure to 130 MPa in the ternary system Na2SO4–NaCl–H2O with boundary binary subsystems of two types. In type 1 subsystems (the NaCl–H2O subsystem in this work), there are no critical phenomena in saturated solutions. Type 2 subsystems (the Na2SO4–H2O subsystem in this work) have terminal critical points p (G = L – \({S_{N{a_2}S{O_4}}}\)) and Q (L1 = L2 – \({S_{N{a_2}S{O_4}}}\)). It was shown that the ternary system contains two regions of three-phase equilibria ((G–L–S) and (L1–L2–S)), divided by a two-phase fluid region (F – \({S_{N{a_2}S{O_4}}}\)), and two types of monovariant critical curves ((G = L – \({S_{N{a_2}S{O_4}}}\)) and (L1 = L2 – \({S_{N{a_2}S{O_4}}}\))). With increasing temperature, these three-phase regions approach each other until the two-phase fluid equilibrium vanishes and the monovariant critical curves meet at a binary homogeneous critical point (G = L–S ⇔ L1 = L2 – \({S_{N{a_2}S{O_4}}}\)) at a maximal temperature of ~495°C and a pressure of ~75 MPa.
About the authors
M. A. Urusova
Kurnakov Institute of General and Inorganic Chemistry
Email: valyashko@igic.ras.ru
Russian Federation, Leninskii pr. 31, Moscow, 119991
V. M. Valyashko
Kurnakov Institute of General and Inorganic Chemistry
Author for correspondence.
Email: valyashko@igic.ras.ru
Russian Federation, Leninskii pr. 31, Moscow, 119991
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