金属热处理 ›› 2025, Vol. 50 ›› Issue (8): 1-7.DOI: 10.13251/j.issn.0254-6051.2025.08.001

• 材料研究 •    下一篇

船用高强球扁钢的连续冷却转变与奥氏体相变动力学分析

祁震1, 梁丰瑞1, 罗小兵1, 柴锋1, 葛启录1, 展之德1, 宋成民1, 罗坤杰2   

  1. 1.钢铁研究总院有限公司 工程用钢研究院, 北京 100081;
    2.苏州热工研究院有限公司, 江苏 苏州 215004
  • 收稿日期:2025-02-27 修回日期:2025-06-11 出版日期:2025-08-25 发布日期:2025-09-10
  • 通讯作者: 罗坤杰,正高级工程师,E-mail:15544838783@163.com
  • 作者简介:祁 震(1995—),男,博士研究生,主要研究方向为船舶及海工用钢材料开发,E-mail:1744616867@qq.com。
  • 基金资助:
    钢铁研究总院有限公司自主投入研发专项基金(事24G60740Z)

Continuous cooling transformation and kinetic analysis of austenite transformation of high strength bulb flat ship steel

Qi Zhen1, Liang Fengrui1, Luo Xiaobing1, Chai Feng1, Ge Qilu1, Zhan Zhide1, Song Chengmin1, Luo Kunjie2   

  1. 1. Research Institute of Engineering Steels, Central Iron and Steel Research Institute Co., Ltd., Beijing 100081, China;
    2. Suzhou Nuclear Power Research Institute Co., Ltd., Suzhou Jiangsu 215004, China
  • Received:2025-02-27 Revised:2025-06-11 Online:2025-08-25 Published:2025-09-10

摘要: 使用Formaster-FⅡ热膨胀仪,结合光学显微镜(OM)、扫描电镜(SEM)和维氏硬度测试,绘制了某船用高强球扁钢的连续冷却转变(CCT)曲线,并对其升温过程中的奥氏体转变进行动力学分析。结果表明,试验钢的Ac1=672 ℃、Ac3=793 ℃。在0.06~38.2 ℃/s冷速范围内,不发生珠光体转变。冷速为0.06~0.3 ℃/s时,发生贝氏体转变,且随冷速提高,贝氏体含量减少;冷却速度为0.8~3.8 ℃/s时,发生马氏体-贝氏体混合相变,随着冷速提高,马氏体含量增加;冷却速度为7.6~38.2 ℃/s时,发生马氏体相变。随着冷却速度的升高,试验钢硬度先快速升高,冷速达到7.6 ℃/s后硬度增加减缓,冷速为38.2 ℃/s时,硬度达最大值359 HV5。利用热膨胀曲线和杠杆定律得到升温过程试验钢的奥氏体转变动力学方程,表明其奥氏体转变为三维方式生长。

关键词: 球扁钢, CCT曲线, 组织转变, 相变动力学

Abstract: Continuous cooling transformation (CCT) curve of a high strength bulb flat ship steel was plotted by using Formaster-FⅡ thermal dilatometer combined with optical microscope (OM), scanning electron microscope (SEM), and Vickers hardness test, and austenite transformation kinetic analysis during the heating process was conducted. The results show that the Ac1 and Ac3 of the tested steel are 672 ℃ and 793 ℃, respectively. Within the cooling rate range of 0.06-38.2 ℃/s, no pearlite transformation is observed. When the cooling rate is 0.06-0.3 ℃/s, bainite transformation occurs, and the bainite volume fraction decreases with the increase of cooling rate. When the cooling rate ranges from 0.8 ℃/s to 3.8 ℃/s, mixed martensite-bainite phase transformation occurs, and the volume fraction of martensite increases with the increase of cooling rate. Martensitic transformation occurs within the cooling rate range of 7.6 ℃/s to 38.2 ℃/s. With the increase of the cooling rate, the hardness of the tested steel first increases rapidly. After the cooling rate reaches 7.6 ℃/s, the hardness increases slowly, and reaches the maximum value of 359 HV5 at the cooling rate of 38.2 ℃/s. The kinetics equation of austenite transformation is derived from the thermal dilatometric curve combined with the lever rule, revealing that the austenite transformation during the heating process follows a three-dimensional growth mechanism.

Key words: bulb flat steel, CCT curve, microstructure transformation, phase transformation kinetics

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