Strengthening Mechanisms and Features of Strain Stages in High-Manganese Austenitic Hadfield Steel

IF 0.9 4区 物理与天体物理 Q4 PHYSICS, CONDENSED MATTER
N. A. Popova, A. A. Klopotov, E. L. Nikonenko, L. I. Trishkina, T. V. Cherkasova, G. G. Volokitin, O. M. Loskutov, V. I. Borodin, A. I. Potekaev
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引用次数: 1

Abstract

The paper presents the study of the deformation effect on high-manganese austenitic Hadfield steel. The dependences of the flow stress and the strain-hardening coefficient on the degree of plastic deformation in uniaxial tension revealed that the linear stage II of strain-hardening at ε ~ 5% can be divided into two substages different in the type of dislocation substructures and values of strain-hardening coefficients. The change in the strain-hardening coefficient correlates with the time when the twinning processes are switched on and the beginning of the transition of the dislocation substructure from one type to another. The following quantitative parameters were determined: the volume fraction of the material caught up by slip and twinning; the volume fractions of the material where twinning develops in one, two, and three systems. Twinning develops most intensively in the range of ε = 5–20%. The involvement of various types of defects (microtwins and dislocations) in the process of deformation does not depend on the method of plastic deformation (tension, rolling). The role of crystallographic texture, which manifests itself in an increase in the Schmid factor during the formation of microtwins, is determined, since microtwinning entails orientational softening and facilitates the sliding process. The presence of minimal and even zero values of the Schmid fa-ctor during twinning was revealed in individual grains. In these grains, the driving force of twinning is the internal stress fields, the occurrence of which is due to the incompatibility of the deformation of neighboring grains.

Abstract Image

高锰奥氏体哈德菲尔德钢应变阶段强化机理及特点
本文研究了高锰奥氏体哈德菲尔德钢的变形效应。流动应力和应变硬化系数与单轴拉伸塑性变形程度的关系表明,ε ~ 5%时的线性应变硬化阶段可分为两个不同位错子结构类型和应变硬化系数值的子阶段。应变硬化系数的变化与孪晶过程开启的时间以及位错子结构从一种类型向另一种类型转变的开始时间有关。确定了以下定量参数:被滑移和孪生捕获的材料的体积分数;在一、二、三体系中形成孪晶的材料的体积分数。孪晶在ε = 5-20%的范围内最为密集。变形过程中涉及的各种类型的缺陷(微孪晶和位错)不依赖于塑性变形(拉伸、轧制)的方法。晶体织构的作用是确定的,它在微孪晶形成过程中表现为施密德系数的增加,因为微孪晶需要取向软化并促进滑动过程。在孪生过程中,个别晶粒的施密德因子存在极小值甚至零值。在这些晶粒中,孪生的驱动力是内部应力场,其发生是由于邻近晶粒变形的不相容。
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来源期刊
Physics of the Solid State
Physics of the Solid State 物理-物理:凝聚态物理
CiteScore
1.70
自引率
0.00%
发文量
60
审稿时长
2-4 weeks
期刊介绍: Presents the latest results from Russia’s leading researchers in condensed matter physics at the Russian Academy of Sciences and other prestigious institutions. Covers all areas of solid state physics including solid state optics, solid state acoustics, electronic and vibrational spectra, phase transitions, ferroelectricity, magnetism, and superconductivity. Also presents review papers on the most important problems in solid state physics.
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