Study of the structural inhomogeneity of bimetal layers at the yield plateau stage

Yulia Li, S. Barannikova, G. Shlyakhova, L. Zuev
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引用次数: 3

Abstract

The paper studies the kinetics of Chernov–Luders band propagation of bimetallic material on the yield plateau at the microscale level. The localization patterns of plastic deformation in the process of uniaxial tension are obtained by noncontact method of recording the fields of displacement vectors. Microstructure of the interfaces studied by atomic force microscopy showed that in the direction of the pearlite steel to the austenitic form there are structural components: the weakened zone of the ferrite layer; hardened section of the ferrite layer dark-pickling layer from the side of austenitic steel. Plastic deformation of a bimetal begins from the nucleation of the Luders band on the boundaries of the bimetal on stress raisers with higher hardness due to the diffusion effect. In the main layer the Luders band is limited to a pair of fronts moving in opposite directions along the bimetal axis with different velocities. The cladding layer does not suppress the formation of Luders bands, leads to an increase in the propagation velocity of Luders band fronts in the base layer and reduces the Luders band propagation in all bimetal layers.The paper studies the kinetics of Chernov–Luders band propagation of bimetallic material on the yield plateau at the microscale level. The localization patterns of plastic deformation in the process of uniaxial tension are obtained by noncontact method of recording the fields of displacement vectors. Microstructure of the interfaces studied by atomic force microscopy showed that in the direction of the pearlite steel to the austenitic form there are structural components: the weakened zone of the ferrite layer; hardened section of the ferrite layer dark-pickling layer from the side of austenitic steel. Plastic deformation of a bimetal begins from the nucleation of the Luders band on the boundaries of the bimetal on stress raisers with higher hardness due to the diffusion effect. In the main layer the Luders band is limited to a pair of fronts moving in opposite directions along the bimetal axis with different velocities. The cladding layer does not suppress the formation of Luders bands, leads to an incre...
屈服平台阶段双金属层结构不均匀性研究
本文研究了微尺度下双金属材料在屈服平台上的Chernov-Luders能带传播动力学。通过记录位移矢量场的非接触方法,得到了单轴拉伸过程中塑性变形的局部化模式。原子力显微镜对界面微观结构的研究表明,在珠光体钢向奥氏体形态转变的方向上存在结构成分:铁素体层减弱区;铁素体层硬化段奥氏体钢侧面的暗酸洗层。双金属的塑性变形开始于双金属在高硬度应力凸起处由于扩散效应而形成的吕德带的形核。在主层中,吕德斯带仅限于沿双金属轴以不同速度向相反方向运动的一对锋面。熔覆层并不抑制吕德带的形成,反而导致基层吕德带锋面的传播速度增加,降低了所有双金属层的吕德带传播。本文研究了微尺度下双金属材料在屈服平台上的Chernov-Luders能带传播动力学。通过记录位移矢量场的非接触方法,得到了单轴拉伸过程中塑性变形的局部化模式。原子力显微镜对界面微观结构的研究表明,在珠光体钢向奥氏体形态转变的方向上存在结构成分:铁素体层减弱区;铁素体层硬化段奥氏体钢侧面的暗酸洗层。双金属的塑性变形开始于双金属在高硬度应力凸起处由于扩散效应而形成的吕德带的形核。在主层中,吕德斯带仅限于沿双金属轴以不同速度向相反方向运动的一对锋面。熔覆层不能抑制吕德斯带的形成,导致…
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