Conferences

THERMODYNAMIC ASSESSMENT OF THE GLASS-FORMING Cu–Ti–Hf SYSTEM

M.A. Turchanin*,
 
P.G. Agraval,
 
G.O. Vodopyanova
 

Donbass State Engineering Academy , st. Academic, 72, Donetsk region, Kramatorsk, 84313, Ukraine
phch@dgma.donetsk.ua
Powder Metallurgy - Kiev: Frantsevich Institute for Problems of Materials Science NASU, 2022, #11/12
http://www.materials.kiev.ua/article/3517

Abstract

In the framework of the CALPHAD method, the thermodynamic assessment of the Cu–Ti–Hf system has been performed for the first time. This assessment considers the existence of homogeneity regions for Cu3Ti2, Cu4Ti3, CuTi, Cu5Hf, Cu51Hf14, and Cu10Hf7 compounds and the formation of a continuous solid solution of Cu(Ti,Hf)2 (γ-phase) in the ternary system. The thermodynamic assessments of the boundary two-component systems and data on phase transformations and mixing enthalpy of melts in the ternary system became the basis for calculations. The Compound Energy Formalism was used to model the thermodynamic properties of intermetallic compounds with а homogeneity region. The associated solution model was used to describe the complex temperature dependence of the thermodynamic properties of melts from the temperature of the existence of equilibrium melts to the glass-formation temperature. Upon the calculations, isothermal sections, vertical sections, projections of the liquidus and solidus surfaces, and the reaction scheme of the phase diagram were presented. The liquid phase participates in eleven four-phase invariant reactions occurring in the temperature range 1138–1541 K. Diagrams of metastable phase transformations involving supercooled Cu–Ti–Hf melts and boundary solid solutions based on pure components were calculated. It is shown that supercooled melts in wide concentration ranges are thermodynamically stable in relation to boundary solid solutions based on pure components. The concentration region of glass formation for Cu–Ti–Hf melts by liquid quenching, predicted by the relative position of the ТοL/Φ and хοL/Φ lines, is xCu ≈ 0.16–0.80.


CONCENTRATION REGIONS OF AMORPHIZATION, METASTABLE PHASE TRANSFORMATIONS, STATE DIAGRAM, THERMODYNAMICS DESCRIPTION OF THE SYSTEM