TY - JOUR
T1 - Non-isothermal crystallization kinetics of Fe75Cr5P9B4C7 metallic glass with a combination of desired merits
AU - Xu, Tao
AU - Jian, Zengyun
AU - Chang, Fange
AU - Zhuo, Longchao
AU - Zhang, Tao
N1 - Publisher Copyright:
© 2018 Elsevier Ltd
PY - 2018/6
Y1 - 2018/6
N2 - The non-isothermal crystallization kinetics of our previously reported Fe75Cr5P9B4C7 metallic glass (MG) was systematically evaluated by X-ray diffraction (XRD), transmission electron microscopy (TEM) and differential scanning calorimeter (DSC). The primary crystalline phases of the present alloy annealed under non-isothermal heating conditions were mainly identified as nanocrystalline α-(Fe,Cr), (Fe,Cr)3P, (Fe,Cr)3C and (Fe,Cr)23(C,B)6 embedded in amorphous matrix by XRD and TEM. The apparent activation energy (E) for characteristic temperatures determined by Kissinger method is similar to that determined by Ozawa method. The Eg for the glass transition temperature is larger than both of the Ex for the onset crystallization temperature and the Ep for the peak temperature, indicating that the energy barrier for the glass transition is higher than that for the crystallization. Furthermore, the local activation energy evaluated by Kissinger-Akahira-Sunose (KAS) method and Ozawa-Flynn-Wall (OFW) method shows similar trend of gradual increase with the progressing of the crystallization process, implying that the improved difficulty of crystallization. Additionally, the local Avrami exponents gradually decreased from the values larger than 2.5 to the values smaller than 2.5, which implies a typical diffusion-controlled growth with variable crystallization mechanisms during the whole process.
AB - The non-isothermal crystallization kinetics of our previously reported Fe75Cr5P9B4C7 metallic glass (MG) was systematically evaluated by X-ray diffraction (XRD), transmission electron microscopy (TEM) and differential scanning calorimeter (DSC). The primary crystalline phases of the present alloy annealed under non-isothermal heating conditions were mainly identified as nanocrystalline α-(Fe,Cr), (Fe,Cr)3P, (Fe,Cr)3C and (Fe,Cr)23(C,B)6 embedded in amorphous matrix by XRD and TEM. The apparent activation energy (E) for characteristic temperatures determined by Kissinger method is similar to that determined by Ozawa method. The Eg for the glass transition temperature is larger than both of the Ex for the onset crystallization temperature and the Ep for the peak temperature, indicating that the energy barrier for the glass transition is higher than that for the crystallization. Furthermore, the local activation energy evaluated by Kissinger-Akahira-Sunose (KAS) method and Ozawa-Flynn-Wall (OFW) method shows similar trend of gradual increase with the progressing of the crystallization process, implying that the improved difficulty of crystallization. Additionally, the local Avrami exponents gradually decreased from the values larger than 2.5 to the values smaller than 2.5, which implies a typical diffusion-controlled growth with variable crystallization mechanisms during the whole process.
KW - Activation energy
KW - Avrami exponent
KW - Crystallization kinetics
KW - Fe-based metallic glass
KW - Non-isothermal
UR - https://www.scopus.com/pages/publications/85043318685
U2 - 10.1016/j.vacuum.2018.03.003
DO - 10.1016/j.vacuum.2018.03.003
M3 - 文章
AN - SCOPUS:85043318685
SN - 0042-207X
VL - 152
SP - 8
EP - 14
JO - Vacuum
JF - Vacuum
ER -