Mechanical Relaxation of a Ti36.2Zr30.3Cu8.3Fe4Be21.2 Bulk Metallic Glass: Experiments and Theoretical Analysis
来源期刊：Acta Metallurgica Sinica2019年第6期
论文作者：J.C.Qiao Y.H.Chen G.J.Lyu K.K.Song J.M.Pelletier Y.Yao
文章页码：726 - 732
摘 要：The dynamic mechanical relaxation behavior of Ti36.2Zr30.3Cu8.3Fe4Be21.2 bulk metallic glass with good glass-forming ability was investigated by mechanical spectroscopy. The mechanical relaxation behavior was analyzed in the framework of quasi-point defects model. The experimental results demonstrate that the atomic mobility of the metallic glass is closely associated with the correlation factor χ. The physical aging below the glass transition temperature T g shows a non-Debye relaxation behavior, which could be well described by stretched Kohlrausch exponential equation. The Kohlrausch exponent βaging reflects the dynamic heterogeneities of the metallic glass. Both concentration of "defects" and atomic mobility decrease caused by the in situ successive heating during the mechanical spectroscopy experiments.
J.C.Qiao1，Y.H.Chen1，G.J.Lyu1，K.K.Song2，J.M.Pelletier3，Y.Yao1
1. School of Mechanics, Civil Engineering and Architecture,Northwestern Polytechnical University2. School of Mechanical, Electrical and Information Engineering,Shandong University (Weihai)3. MATEIS, UMR CNRS5510, Bat.B.Pascal, INSA-Lyon,Université de Lyon
摘 要：The dynamic mechanical relaxation behavior of Ti36.2Zr30.3Cu8.3Fe4Be21.2 bulk metallic glass with good glass-forming ability was investigated by mechanical spectroscopy. The mechanical relaxation behavior was analyzed in the framework of quasi-point defects model. The experimental results demonstrate that the atomic mobility of the metallic glass is closely associated with the correlation factor χ. The physical aging below the glass transition temperature T g shows a non-Debye relaxation behavior, which could be well described by stretched Kohlrausch exponential equation. The Kohlrausch exponent βaging reflects the dynamic heterogeneities of the metallic glass. Both concentration of "defects" and atomic mobility decrease caused by the in situ successive heating during the mechanical spectroscopy experiments.
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