Peculiarities of steel hardening under deformation conditions with external influence of a magnetic field

C. Dong, М. Kraiev
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Abstract

The strain resistance of a metal, its intensity of hardening, directly depends on the evolution of defects in the crystal lattice. The positive influence of a magnetic field (MF) on the movement of dislocations and their interaction with stoppers (magnetoplastic effect) is known. For the practical use of MF in forging technologies, generalized data on the strengthening of metals during plastic deformation are required. The results of using a constant MF with induction up to 1,2 T in the processes of testing samples for tension and compression were studied. Tensile tests were carried out on samples of steels St3, 20, U8, 40Cr, 09Cr16Ni4Nb, X10CrNiTi18-10, copper M3 and compression tests on steels St3, 09Cr16Ni4Nb, X10CrNiTi18-10, copper M3. Curves of metal hardening during deformation are plotted in the coordinates flow stress – logarithmic strain. The flow stress is determined by the ratio of the load to the cross-sectional area of the sample valid for a given moment of testing under uniform deformation. The change in flow stress of metals is described by the power function of the Ludwik-Hollomon equation. In tension and compression of ferromagnetic steels St3, 20, 40Cr, U8 and 09Cr16Ni4Nb, the impact of MF leads to an increase in the intensity of their hardening. This is most evident in hardened or high-strength steels. But for St3 steel softened by annealing, the effect is the opposite - in MF the intensity of hardening is somewhat less. Tension in MF of paramagnetic steel X10CrNiTi18-10 showed an increase in the intensity of hardening, but compression showed its decrease. Tension and compression of M3 copper in MF occur with a slight decrease in the intensity of hardening. The experiments carried out revealed the main effect of MF at the initial stage of deformation. The hardening curves were divided into straight and parabolic sections with the hardening coefficients determined for each of them. The main effect of MT on the primary stage of linear hardening has been revealed, where a decrease in the intensity of hardening (St3, 40Cr, X10CrNiTi18-10, M3), an increase (St3 and X10CrNiTi18-10) or a reduction (St3 annealed) in the duration of this stage is observed. Keywords: magnetoplasticity, tension, compression, hardening, stress, strain.
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磁场外部影响下变形条件下钢硬化的特殊性
金属的应变电阻及其硬化强度直接取决于晶格中缺陷的演变。众所周知,磁场(MF)对位错运动及其与挡块的相互作用(磁塑效应)具有积极影响。为了在锻造技术中实际使用磁场,需要有关塑性变形期间金属强化的通用数据。我们研究了在拉伸和压缩样品测试过程中使用感应高达 1.2 T 的恒定磁场的结果。拉伸试验在 St3、20、U8、40Cr、09Cr16Ni4Nb、X10CrNiTi18-10 和 M3 铜样品上进行,压缩试验在 St3、09Cr16Ni4Nb、X10CrNiTi18-10 和 M3 铜样品上进行。变形过程中的金属硬化曲线以流动应力-对数应变为坐标绘制。流动应力是在均匀变形的情况下,在给定测试时刻有效的载荷与试样横截面积的比值。金属流动应力的变化由 Ludwik-Hollomon 方程的幂函数描述。在拉伸和压缩铁磁钢 St3、20、40Cr、U8 和 09Cr16Ni4Nb 时,流动应力的影响导致其硬化强度增加。这在淬火钢或高强度钢中最为明显。但对于通过退火软化的 St3 钢来说,效果则恰恰相反--在中频情况下,硬化强度略有降低。顺磁钢 X10CrNiTi18-10 的中频拉伸显示硬化强度增加,但压缩显示硬化强度降低。在中频中拉伸和压缩 M3 铜时,硬化强度略有下降。所进行的实验表明,MF 在变形的初始阶段具有主要影响。硬化曲线分为直线段和抛物线段,并分别确定了硬化系数。MT对线性硬化初级阶段的主要影响已经显现,在这一阶段,硬化强度降低(St3、40Cr、X10CrNiTi18-10、M3),硬化持续时间增加(St3 和 X10CrNiTi18-10)或缩短(St3 退火)。关键词:磁塑性、拉伸、压缩、硬化、应力、应变。
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