✦ LIBER ✦

Phase diagrams with critical and tricritical liquid phase solution points in a ternary system

✍ Scribed by K. A. Khaldoyanidi

Book ID: 110184302
Publisher: International Academic Publishing Co (Nauka/Interperiodica)
Year: 2008
Tongue: English
Weight: 166 KB
Volume: 82
Category: Article
ISSN: 0036-0244
DOI: 10.1134/s0036024408120017

No coin nor oath required. For personal study only.

📜 SIMILAR VOLUMES

Liquid-liquid phase splitting—III: Azeot

Liquid-liquid phase splitting—III: Azeotropy and critical solution temperature in ternary systems

✍ Jaime Wisniak 📂 Article 📅 1984 🏛 Elsevier Science 🌐 English ⚖ 325 KB

Model melting diagrams of ternary system

Model melting diagrams of ternary systems with a lower critical liquid stratification point

✍ K. A. Khaldoyanidi 📂 Article 📅 2007 🏛 International Academic Publishing Co (Nauka/Interp 🌐 English ⚖ 155 KB

Pressure-induced tricritical point and c

Pressure-induced tricritical point and critical behavior near the points of phase-diagram wings in a CoS2ferromagnet

✍ É. Z. Valiev; F. S. Shemet’ev 📂 Article 📅 2004 🏛 SP MAIK Nauka/Interperiodica 🌐 English ⚖ 53 KB

Reentrant phase transition and tricritic

Reentrant phase transition and tricritical points in a quantum transverse spin system with a random field

✍ Y.Q. Ma; Y.G. Ma 📂 Article 📅 1993 🏛 Elsevier Science 🌐 English ⚖ 251 KB

Phase diagrams of degenerate states in t

Phase diagrams of degenerate states in ternary metal and metal chalcogenide systems with solid solutions

✍ K. A. Khaldoyanidi 📂 Article 📅 2007 🏛 SP MAIK Nauka/Interperiodica 🌐 English ⚖ 251 KB

Phase diagrams and multicritical points

Phase diagrams and multicritical points in the ternary mixed-spin alloy with a single-ion anisotropy

✍ J. Dely; A. Bobák 📂 Article 📅 2006 🏛 John Wiley and Sons 🌐 English ⚖ 165 KB

## Abstract The phase diagram of the __AB~p~C__ ~1–__p__~ ternary alloy consisting of different Ising spins __S^A^__ = 3/2, __S^B^__ = 2, and __S^C^__ = 5/2 in the presence of a single‐ion anisotropy is investigated by the use of a mean‐field theory. At finite temperature by changing values of the