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Hot compression deformation behavior and microstructure evolution rule of a high-speed railway axle steel

机译:高速铁路车轴钢的热压缩变形行为及组织演变规律

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The high performance of high-speed railway axle (HSRA) depends on the stress-strain state and microstructure formed in the hot processes, it is necessary to investigate the deformation behavior and microstructure evolution during hot uniaxial compression. Hot compression test was performed on specimen of a HSRA steel 25CrMo4 at a deformation temperature of 1040-1160oC at a strain rate of 1.0-10.0 /s using a Gleeble thermal mechanical simulator. During hot compression test, samples were compressed to different true strain: 0, 0.2, 0.4, 0.6 and 0.8. Hot compressive deformation behaviors and effects of processing parameters, including forming temperature, strain rate and deformation degree, on microstructure evolution of HSRA steel 25CrMo4 are investigated and studied by metallurgical analysis. Experiments results show that the peak value of flow stress increases about 30 MPa at a certain deformation temperature when the strain rate increases from 1.0 /s to 10.0 /s. At a certain strain rate, the peak value of flow stress increases about 20-30 MPa when the forming temperature decreases about 60oC. The average grain sizes increases with the increasing of forming temperature at a certain strain rate and a given strain. For a given forming temperature, grain size decreased before the critical strain of 0.4 and increased after strain of 0.4 due to grain growth, especially at lower strain rate. Therefore, grain size at lower strain rate is larger than that at higher strain rate when true strain reached 0.8.
机译:高速铁路车轴(HSRA)的高性能取决于热加工过程中形成的应力-应变状态和微结构,有必要研究热单轴压缩过程中的变形行为和微结构演变。使用Gleeble热力学模拟器在HSRA钢25CrMo4的试样上以104-1160℃的变形温度在1.0-10.0 / s的应变速率下进行了热压缩试验。在热压缩测试期间,样品被压缩到不同的真实应变:0、0.2、0.4、0.6和0.8。通过冶金分析研究了热压缩变形行为以及成形温度,应变速率和变形程度等工艺参数对HSRA钢25CrMo4组织演变的影响。实验结果表明,当应变速率从1.0 / s增加到10.0 / s时,在一定的变形温度下,流动应力的峰值增加约30 MPa。在一定的应变速率下,当成形温度降低约60℃时,流动应力的峰值增加约20-30 MPa。在一定的应变速率和给定的应变下,平均晶粒尺寸随着成形温度的增加而增加。对于给定的成形温度,由于晶粒长大,特别是在较低的应变速率下,晶粒尺寸在临界应变0.4之前减小,而在应变0.4之后则增大。因此,当真实应变达到0.8时,较低应变速率下的晶粒尺寸大于较高应变速率下的晶粒尺寸。

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