Comparison between the Lüders and Portevin–Le Chatelier bands in the low-strain-rate tensile testing of ultralow-carbon ferritic steel

IF 1.6 4区 材料科学 Q2 METALLURGY & METALLURGICAL ENGINEERING
Eibun Kyo, Seung-Yong Lee, Ryota Nagashima, Nobuo Nakada, Fusae Shiimori, Nobusuke Kariya, Shinjiro Kaneko
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Abstract

In ferritic steels, solute carbon (C) causes two types of discontinuous stress fluctuations that are accompanied by local deformation bands in the stress–strain curves. One is the yield drop with the Lüders band at yielding, and the other is the serrated flow stress with Portevin–Le Chatelier (PLC) bands during the strain hardening stage, that is, the PLC effect. Lüders band and PLC bands can be explained by static strain aging and dynamic strain aging, SSA and DSA, respectively. These difference in strain aging mechanics distinguish the Lüders band and PLC bands and qualitatively explain when they appear in the stress–strain curve at the yielding and strain-hardening stages. Nevertheless, Lüders band and PLC effect occur in carbon steels at room temperature and 373–473 K, respectively. Therefore, fundamental difference between these bands remains unclear because it is difficult to compare them under the same tensile conditions. In this study, low-strain-rate tensile tests were performed on ultralow-carbon ferritic steel at ambient temperature to compare the bands under the same deformation conditions. In addition to the Lüders band, the formation and propagation of PLC bands were observed at strain rates lower than 1.0 × 10-4 s-1, and the PLC effect became more pronounced as the strain rate decreased and the carbon content increased. Furthermore, local strain analysis using digital image correlation revealed that the dislocation movement was much faster than C diffusion only in the Lüders band, which is attributed to the difference in the strain-aging mechanism.

超低碳铁素体钢低应变速率拉伸试验中 Lüders 带和 Portevin-Le Chatelier 带的比较
在铁素体钢中,溶质碳(C)会导致两种类型的不连续应力波动,并在应力-应变曲线中伴有局部变形带。一种是屈服时带有吕德斯带的屈服下降,另一种是应变硬化阶段带有波特文-勒夏特列(PLC)带的锯齿流动应力,即 PLC 效应。吕德斯带和 PLC 带可分别用静态应变时效和动态应变时效(SSA 和 DSA)来解释。应变时效力学的这些差异区分了 Lüders 带和 PLC 带,并定性地解释了它们在屈服阶段和应变硬化阶段的应力-应变曲线中出现的时间。然而,Lüders 带和 PLC 效应分别出现在室温和 373-473 K 的碳钢中。因此,由于很难在相同的拉伸条件下对它们进行比较,这些带之间的根本区别仍不清楚。本研究在环境温度下对超低碳铁素体钢进行了低应变速率拉伸试验,以比较相同变形条件下的带。除 Lüders 带外,在应变速率低于 1.0 × 10-4 s-1 时,还观察到 PLC 带的形成和传播,并且随着应变速率的降低和碳含量的增加,PLC 效应更加明显。此外,利用数字图像相关性进行的局部应变分析表明,只有在吕德斯带中,位错运动比 C 扩散快得多,这归因于应变时效机制的不同。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Isij International
Isij International 工程技术-冶金工程
CiteScore
3.40
自引率
16.70%
发文量
268
审稿时长
2.6 months
期刊介绍: The journal provides an international medium for the publication of fundamental and technological aspects of the properties, structure, characterization and modeling, processing, fabrication, and environmental issues of iron and steel, along with related engineering materials.
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