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金属学报  2017, Vol. 53 Issue (6): 733-742    DOI: 10.11900/0412.1961.2016.00509
  本期目录 | 过刊浏览 |
全淬透圆柱件淬火应力的有限元模拟及实验验证
刘玉1,秦盛伟1,左训伟1,陈乃录2(),戎咏华1
1 上海交通大学材料科学与工程学院 上海 200240
2 上海交通大学材料科学与工程学院上海市激光制造与材料改性重点实验室 上海 200240
Finite Element Simulation and Experimental Verification of Quenching Stress in Fully Through-Hardened Cylinders
Yu LIU1,Shengwei QIN1,Xunwei ZUO1,Nailu CHEN2(),Yonghua RONG1
1 School of Materials Science and Engineering, Shanghai Jiao Tong University, Shanghai 200240, China
2 Shanghai Key Laboratory of Materials Laser Processing and Modification, School of Materials Science and Engineering, Shanghai Jiao Tong University, Shanghai 200240, China
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摘要: 

利用温度场、组织场和应力场相互耦合的数学模型对直径60 mm的40CrNiMo水淬圆棒的淬火应力进行研究。结果表明,有限元模拟的淬火应力及其分布与XRD测量结果相符,论证了所运用的温度场、组织场和应力场相互耦合的数学模型(包括建立的相变塑性函数)的正确性。通过计算机模拟分离了淬火马氏体钢中的热应力和组织应力,揭示了不同直径淬透圆棒试样的应力分布规律及其起因以及不同淬火介质对淬火应力的影响规律。

关键词 全淬透圆柱件淬火应力热应力组织应力有限元模拟    
Abstract

Quenching is one of the most important heat-treatment processes for improving the mechanical properties of steel components in manufacture industry. The quenching stress is a source of cracking, which is frequently detrimental to steel properties. Therefore, the investigation of quenching stress is very important for the control of distortion, cracking and residual stress distributions of components. In the study of quenching stress, the measurement of stress distribution is necessary to the stress analysis and design of quenching process. However, in most cases, the cracking of a quenched component is caused by transient stress during quenching, while experiment can only measures the final internal stress (residual stress), rather than transient stress. As a result, the measurement of residual stress associated with finite element simulation (FES) has been a mainstream direction in the investigation of quenching stress. In this work, a full through-hardened 40CrNiMo cylinder with 60 mm diameter was water-quenched, and cooling curves at three positions along the radius of cylinder were measured. Then, an optimized heat transfer coefficient as a function of surface temperature was obtained by fitting with the measured cooling curves using the trial and error method. Based on an exponent-modified (Ex-Modified) normalized function describing transformation plasticity kinetics proposed, the thermo-elasto-plastic constitutive equations were deduced. The commercial finite element software, Abaqus/Standard, was used to solve the coupled temperature field, microstructure field and stress (strain) field. The results indicate that the quenching stress and its distribution predicted by FES is well consistent with those measured by XRD, which verified that the models employed in coupling of thermal field, phase transformation field and stress field including transformation plasticity function proposed are correct. Meanwhile, the features of residual stress distribution were revealed that compressive stress exists in the core and surface of cylinder and the maximum tensile stress exists at subsurface. The separated calculation of thermal stress and phase transformation stress by FES reveals the origin of residual stress distribution feature in quenched cylinders, that is, the relative higher phase transformation compressive stress and lower tensile thermal stress at the core of cylinder make the residual stress to be compressive, while at the surface of cylinder the compressive stress is predominantly from thermal stress, because it is much larger than the tensile stress caused by phase transformation stress. The tangential residual stress distributions in cylinders with several diameters from 3 mm to 100 mm were predicted by FES, and the results indicate that when diameter is less than 5 mm, the tensile stress at the surface increases with increasing diameter until to 5 mm, then decreases with increasing diameter to 20 mm, finally the tensile stress becomes compressive stress. Besides, with the increase of diameter, maximum tensile stress shifts from the surface to the location of 0.6 radius. The effects of different quenching media on quenching stress were also investigated by FES. The results demonstrated that although there is compressive stress at surface of cylinder quenched in water or salt solution, the maximum stress locates the subsurface, meaning that cracking easily occurs at the subsurface, which is consistent with cracking in practical components. This work is helpful for the analysis of cracking from quenching stress in components with different sizes and under different quenching media.

Key wordsfully through-hardened cylinder    quenching stress    thermal stress    phase transformation stress    finite element simulation
收稿日期: 2016-11-14      出版日期: 2017-02-27
:     
基金资助:国家自然科学基金项目No.51371117

引用本文:

刘玉, 秦盛伟, 左训伟, 陈乃录, 戎咏华. 全淬透圆柱件淬火应力的有限元模拟及实验验证[J]. 金属学报, 2017, 53(6): 733-742.
Yu LIU, Shengwei QIN, Xunwei ZUO, Nailu CHEN, Yonghua RONG. Finite Element Simulation and Experimental Verification of Quenching Stress in Fully Through-Hardened Cylinders. Acta Metall, 2017, 53(6): 733-742.

链接本文:

http://www.ams.org.cn/CN/10.11900/0412.1961.2016.00509      或      http://www.ams.org.cn/CN/Y2017/V53/I6/733

图1  淬火过程简化后的耦合关系
图2  试样不同位置的冷却曲线测量与计算结果的比较,及修正后的换热系数与文献[32]数据的比较
图3  奥氏体、贝氏体和马氏体的热膨胀曲线
图4  直径60 mm的40CrNiMo圆柱件水淬后1/2半径处和心部的显微组织OM像
图5  40CrNiMo圆柱件水淬后组织体积分数(计算和测量)和硬度(测量)的截面分布
图6  直径60 mm的40CrNiMo圆棒水淬后轴向及切向应力的截面分布
图7  直径60 mm的40CrNiMo圆棒水淬时心部、表面及距表面10 mm位置处的切向应力变化过程
图8  直径60 mm的40CrNiMo圆棒水淬热应力、组织应力及残余应力计算结果的比较
图9  不同直径全淬透圆棒工件水淬后的切向残余应力、热应力和组织应力分布
图10  直径50 mm的全淬透试样分别在空气、水、80 ℃油和10%NaCl水溶液淬火后的切向残余应力、热应力和组织应力分布
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