Evaluation of thermal stability and isochronal crystallization kinetics in the Ti40Zr25Ni8Cu9Be18 bulk metallic glass

被引:38
|
作者
Hu, Xinxin [1 ]
Qiao, Jichao [1 ,2 ]
Pelletier, Jean M. [2 ]
Yao, Yao [1 ]
机构
[1] Northwestern Polytech Univ, Sch Mech Civil Engn & Architecture, Xian 710072, Peoples R China
[2] Univ Lyon, MATEIS, UMR CNRS5510, INSA Lyon, F-69621 Villeurbanne, France
关键词
Bulk metallic glass; Thermal stability; Non-isothermal crystallization; Differential scanning calorimety; DIFFERENTIAL SCANNING CALORIMETRY; HEATING RATES VHR; NONISOTHERMAL CRYSTALLIZATION; ACTIVATION-ENERGY; AMORPHOUS-ALLOYS; FORMING ABILITY; PHASE-TRANSFORMATIONS; SUPERCOOLED LIQUID; CHALCOGENIDE GLASS; NUCLEATION;
D O I
10.1016/j.jnoncrysol.2015.10.018
中图分类号
TQ174 [陶瓷工业]; TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
The thermal stability of Ti40Zr25Ni8Cu9Be18 bulk metallic glass was studied by differential scanning calorimetry (DSC). Under non-isothermal heating process, the results indicate that the Ti40Zr25Ni8Cu9Be18 bulk metallic glass show two crystallization processes. X-ray diffraction (XRD) was conducted at room temperature and annealed temperature to examine the phase nature. Several theoretical models were used to analyze the apparent activation energies for characteristic temperatures (i.e. the glass transition temperature, the onset temperature of the crystallization, etc.). The results show that the apparent activation energies for characteristic temperatures in the Ti40Zr25Ni8Cu9Be18 bulk metallic glass by Kissinger model, Flynn-Wall-Ozawa model, Augis-Bennett model and Gao-Wang model are in good agreement with each other. The average values of the Avrami exponent n in the first and the second crystallization processes for the Ti40Zr25Ni8Cu9Be18 bulk metallic glass are around 1.41 and 2.47, respectively. The apparent activation energies are determined by different isoconversion methods, the values are close to each other in both crystallization processes. (C) 2015 Elsevier B.V. All rights reserved.
引用
收藏
页码:254 / 264
页数:11
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