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首页> 外文期刊>Intermetallics >Superplastic deformation behavior of Zr_(41.25)Ti_(13.75)Ni_(10)Cu_(12.5)Be_(22.5) bulk metallic glass in the supercooled liquid region
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Superplastic deformation behavior of Zr_(41.25)Ti_(13.75)Ni_(10)Cu_(12.5)Be_(22.5) bulk metallic glass in the supercooled liquid region

机译:Zr_(41.25)Ti_(13.75)Ni_(10)Cu_(12.5)Be_(22.5)大块金属玻璃在过冷液体区的超塑性变形行为

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This paper presents the tensile deformation behavior of Zr_(41.25)Ti_(13.75)Ni_(10)Cu_(12.5)Be_(22.5) (at percent) bulk metallic glass in the supercooled liquid region. Isothermal tensile tests were earned out at four characteristic temperatures of 616, 636, 656 and 676 K which are in the range from glass transition temperature (approx 616 K) to onset crystallization temperature (approx 690 K). The results show that the superplastic flow behaviors of the material (flow stress and elongation to fracture) vary, depending strongly on the test temperatures and initial strain-rates. At a given temperature, the elongation first increases and then decreases with the initial strain-rate increasing, and the maximum elongation was found to be as high as 1625 percent at the temperature of 656 K with the strain-rate of 7.6 X 10~(-3) s~(-1). DSC analysis shows the crystallized volume fraction in the deformed section is always higher than that of the undeformed section in the specimens. The maximum elongation always corresponds to the maximum crystallized volume fraction. Nanocrystals homogeneously embedded in the amorphous matrix of the deformed specimens were observed by transmission electron microscope. It is conjectured that the nanocrystallization was induced by the flow stress and environmental temperature.
机译:本文介绍了Zr_(41.25)Ti_(13.75)Ni_(10)Cu_(12.5)Be_(22.5)(at%)大块金属玻璃在过冷液体区域的拉伸变形行为。在616、636、656和676 K的四个特征温度下进行了等温拉伸试验,这些温度在从玻璃化转变温度(约616 K)到开始结晶温度(约690 K)的范围内。结果表明,材料的超塑性流动行为(流动应力和断裂伸长率)变化很大,这主要取决于测试温度和初始应变率。在给定温度下,伸长率先随初始应变率的增加而增加,然后减小,在656 K的温度下,应变率为7.6 X 10〜(),最大伸长率高达1625%。 -3)s〜(-1)。 DSC分析表明,变形部分的结晶体积分数总是高于试样中未变形部分的结晶体积分数。最大伸长率始终对应于最大结晶体积分数。用透射电子显微镜观察了均匀地包埋在变形试样的非晶基质中的纳米晶体。据推测,纳米晶化是由流动应力和环境温度引起的。

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