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Acta Metall Sin  2017, Vol. 53 Issue (7): 817-823    DOI: 10.11900/0412.1961.2016.00322
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Nanoindentation Creep Behavior of U65Fe30Al5 Amorphous Alloy
Hongyang XU,Haibo KE,Huogen HUANG,Pei ZHANG,Pengguo ZHANG,Tianwei LIU()
Institute of Materials, China Academy of Engineering Physics, Jiangyou 621907, China
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Abstract  

Uranium is a valuable nuclear fuel material, but this application is unavoidably handicapped by the easy creep behavior of the metal caused by the combination of stress and irradiation in nuclear reactor. Uranium-based amorphous alloys, as a kind of potential new materials in the nuclear industry, would be challenged by this issue when used in such situation. However, creep properties of these materials have not been reported in the previous studies. In order to preliminarily investigate the creep phenomenon derived from stress function, this work is performed to study the ambient creep behavior of a new amorphous alloy U65Fe30Al5. This alloy was tested by using a nanoindentation technique under different peak loads and loading rates. The results indicate that the creep displacement gradually increases with either the peak load or the loading rate in equal creeping time, but this tendency vanishes when exceeding a critical loading rate. The fitting based on an empirical creep equation reveals that the stress exponent of the alloy ascends when raising the peak load, and firstly declines with the loading rate and then keeps constant above the critical rate. Compared with conventional crystalline alloys, the U-Co-Al alloy shows a larger stress exponent, reflecting the possible existence of rich free volume in the amorphous alloy.

Key words:  amorphous alloy      uranium alloy      nanoindentation      creep      stress exponent     
Received:  21 July 2016     
Fund: Supported by National Natural Science Foundation of China (No.51501169), National Defense Basic Scientific Research (No.B1520133007) and Scientific and Technological Development Foundation of China Academy of Engineering Physics (Nos.2013A0301015 and 2014B0302047)

Cite this article: 

Hongyang XU,Haibo KE,Huogen HUANG,Pei ZHANG,Pengguo ZHANG,Tianwei LIU. Nanoindentation Creep Behavior of U65Fe30Al5 Amorphous Alloy. Acta Metall Sin, 2017, 53(7): 817-823.

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https://www.ams.org.cn/EN/10.11900/0412.1961.2016.00322     OR     https://www.ams.org.cn/EN/Y2017/V53/I7/817

Fig.1  Loading function and ideal characteristic curves for nanoindentation creep (S—contact stiffness, h—indentation depth, F—load, hmax—maximum indentation depth, hf—permanent deformation depth after fully unloading, t—time, σ—stress)

(a) load-time curve (b) load-depth curve (c) standard creep depth-time curve

Fig.2  XRD spectrum of U65Fe30Al5 amorphous alloy
Fig.3  Load-depth (a) and creep displacement-time (b) curves during 30 s nanoindentation creeping under different peak loads (The curves in the Fig.3b are offset from the origin points of the creep process)
Fig.4  Load-depth (a) and creep displacement-time (b) curves during 30 s nanoindentation creeping under different loading rates (Curves in Fig.4a are translation-transformed)
Fig.5  Variation of creep displacement versus peak load (a) and loading rate (b) during the nanoindentation creeping of U65Fe30Al5 amorphous alloy
Fig.6  Experimental and fitting curve (Eq.(3)) (a) and the variation of stress exponent derived from stress-strain rate relationship curve (b) during the nanoindentation creeping of U65Fe30Al5 amorphous alloy (h0—initial creep displacement, t0—initial creep time, a and k—fitting parameters)
Fig.7  Curves of stress exponent-peak load (a) and stress exponent-loading rate (b) during the steady creeping of U65Fe30Al5 amorphous alloy(n—stress exponent)
Composition Material type Peak load mN Creep time / s Loading rate mNs-1 Stress exponent
U65Fe30Al5 Amorphous 100 30 20 89
Ti40Zr25Ni3Cu12Be20[18] Amorphous 100 2000 0.1 5
Ta film[24] Amorphous 8 40 5 78.7
Fused quartz[20] Glass 69.4 95 - 85
B6O[26] Polycrystalline 100 15 200 0.14
Table 1  Creep stress exponents for different materials in nanoindentation tests
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