Mg-Cu-Y-Al块状非晶合金的制备及性能研究

N. Pryds, M. Eldrup, M. Ohnuma, A. Pedersen, J. Hattel, S. Linderoth
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引用次数: 32

摘要

采用一种相对简单的技术,在铜楔型模具中快速冷却熔体,制备了块状非晶态(mg1yal y) 60cu30y10合金。记录了熔体冷却和凝固过程中的温度与时间的关系,并与该过程的时空数值模拟进行了比较。可以得出结论,凝固样品的非晶部分与模具之间保持了良好的热接触,而样品的结晶部分与模具之间的接触相当差,这可能是由于结晶过程中晶体-模具界面上出现了狭窄的间隙。当Al含量在0 ~ y = 10%范围内增加时,最大非晶层厚度从~ 3mm减小到零。采用x射线衍射(XRD)和差示扫描量热法(DSC)研究了不同合金成分和退火温度下初始非晶相的微观结构演变。在退火至过冷液态(441 K)时,不含Al的试样基本保持无定形,而纳米颗粒形成,并且在含有少量Al的试样中在较高温度下保持稳定。不含Al的合金在没有纳米颗粒形成的情况下明显结晶。通过DSC数据和温度与时间测量的结合,实验确定了非晶Mg 60 Cu 30 y10试样形成的临界冷却速率为60-150 K/s,与文献估计一致。y = 2%时非晶材料的维氏硬度(hv)高于y = 0时的维氏硬度(~ 360 kg/mm 2)。在结晶过程中,后一种材料的硬度增加到400kg / mm2,而前者的硬度没有变化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Preparation and Properties of Mg–Cu–Y–Al Bulk Amorphous Alloys
Bulk amorphous (Mg 1-y Al y ) 60 Cu 30 Y 10 alloys were prepared using a relatively simple technique of rapid cooling of the melt in a copper wedge mould. The temperature vs. time was recorded during the cooling and solidilication process of the melt and compared with a spacial and temporal numerical simulation of that process. It is concluded that good thermal contact is maintained between the amorphous part of the solidified sample and the mould, while a rather poor contact develops between the crystalline part of the sample and the mould, probably due to the appearance of a narrow gap at the crystal-mould interface during crystallisation. The maximum amorphous layer thickness decreases from ∼3 mm to zero when the Al content increases in the range from 0 to about y = 10%. The evolution of the microstructure of the initially amorphous phase was examined by x-ray diffraction (XRD) and differential scanning calorimetry (DSC) for different alloy compositions and annealing temperatures. On annealing into the supercooled liquid state (441 K), specimens with no Al content remain basically amorphous while nanoparticles are formed and remain stable also at higher temperatures in specimens containing a few percent Al. The alloy with no Al crystallises apparently without the formation of nanoparticles. The critical cooling rate for the formation of an amorphous Mg 60 Cu 30 Y 10 specimen was determined experimentally by a combination of DSC data and temperature vs. time measurements to be 60-150 K/s, in agreement with estimates from the literature. The Vickers hardness (H V ) of the amorphous material for y = 2% is higher (∼360 kg/mm 2 ) than for y = 0 (∼290 kg/mm 2 ). On crystallisation the hardness of the latter material increases to the 400 kg/mm 2 level while the hardness of the former does not change.
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