TY - JOUR
T1 - Evaluation of thermal stability and isochronal crystallization kinetics in the Ti40Zr25Ni8Cu9Be18 bulk metallic glass
AU - Hu, Xinxin
AU - Qiao, Jichao
AU - Pelletier, Jean M.
AU - Yao, Yao
N1 - Publisher Copyright:
© 2015 Elsevier B.V.
PY - 2016/1/1
Y1 - 2016/1/1
N2 - 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.
AB - 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.
KW - Bulk metallic glass
KW - Differential scanning calorimetry
KW - Non-isothermal crystallization
KW - Thermal stability
UR - http://www.scopus.com/inward/record.url?scp=84951754789&partnerID=8YFLogxK
U2 - 10.1016/j.jnoncrysol.2015.10.018
DO - 10.1016/j.jnoncrysol.2015.10.018
M3 - 文章
AN - SCOPUS:84951754789
SN - 0022-3093
VL - 432
SP - 254
EP - 264
JO - Journal of Non-Crystalline Solids
JF - Journal of Non-Crystalline Solids
ER -