Copper–Palladium Phase Diagram

Phase equilibria in the copper–palladium system are extrapolated to absolute zero of temperature subject to the third law of thermodynamics. The continuous solid solution with a FCC structure that crystallizes from melt experiences ordering to yield two intermetallic phases (Kurnakov phases), whose...

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Published inRussian journal of inorganic chemistry Vol. 66; no. 6; pp. 891 - 893
Main Authors Fedorov, P. P., Shubin, Yu. V., Chernova, E. V.
Format Journal Article
LanguageEnglish
Published Moscow Pleiades Publishing 01.06.2021
Springer Nature B.V
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Summary:Phase equilibria in the copper–palladium system are extrapolated to absolute zero of temperature subject to the third law of thermodynamics. The continuous solid solution with a FCC structure that crystallizes from melt experiences ordering to yield two intermetallic phases (Kurnakov phases), whose compositions shrink to CuPd and Cu 3 Pd stoichiometries as temperature lowers. As temperature raises, palladium partially occupies copper sites in the intermetallic phases. Ordering obeying a second-order phase transition to yield a phase whose idealized composition may be formulated as Cu 21 Pd 7 . When in a solid state, the system forms an eutectoid at 390°C and 30 at % Pd and two dystectoids with coordinates of 510°C, 15 at % Pd and 600°C, 40 at % Pd.
Bibliography:ObjectType-Article-1
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content type line 14
ISSN:0036-0236
1531-8613
DOI:10.1134/S0036023621050053