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石墨化钢石墨化过程的金相分析及其动力学方程
引用本文:张永军,李新鹏,王九花,刘靖,韩静涛. 石墨化钢石墨化过程的金相分析及其动力学方程[J]. 工程科学学报, 2022, 44(2): 228-234. DOI: 10.13374/j.issn2095-9389.2021.01.10.004
作者姓名:张永军  李新鹏  王九花  刘靖  韩静涛
作者单位:北京科技大学材料科学与工程学院,北京 100083
基金项目:北京市自然科学基金资助项目(2172035)
摘    要:在650、680和710 ℃不同温度条件下对碳质量分数为0.66%的淬火高碳钢进行了石墨化处理,并利用场发射扫描电子显微镜、电子探针、X-射线衍射仪和透射电子显微镜对其石墨化过程的组织进行金相分析,以及利用组织转变动力学理论,绘制了其石墨化过程的动力学曲线,并建立了相应的动力学方程。研究结果显示:在石墨化过程中,淬火马氏体首先向析出碳化物的稳定状态转变,且在碳化物为渗碳体Fe3C时,石墨粒子析出速度开始明显增加;基体组织中针叶状α-Fe发生再结晶,由等轴状铁素体逐步代替针叶状的α-Fe;铁素体中的碳含量随着石墨化时间的延长而逐步降低,即由过饱和状态转变为稳定态,碳含量在石墨粒子中突变增为峰值,而铁含量则突变降为谷值,由此表明,渗碳体分解的碳向石墨核心扩散,铁自石墨核心处扩散出来,而形成石墨粒子;石墨粒子面积分数随时间变化的曲线呈S形状,即该动力学过程符合动力学模型JMAK(Johnson-Mehl-Avrami-Kolmogorov)方程,且该方程中的n值为1.5~1.7。 

关 键 词:石墨化钢   石墨粒子   铁素体   金相分析   JMAK(Johnson-Mehl-Avrami-Kolmogorov)方程
收稿时间:2021-01-10

Metallographic analysis and kinetic equation of the graphitization process of graphitized steel
ZHANG Yong-jun,LI Xin-peng,WANG Jiu-hua,LIU Jing,HAN Jing-Tao. Metallographic analysis and kinetic equation of the graphitization process of graphitized steel[J]. Chinese Journal of Engineering, 2022, 44(2): 228-234. DOI: 10.13374/j.issn2095-9389.2021.01.10.004
Authors:ZHANG Yong-jun  LI Xin-peng  WANG Jiu-hua  LIU Jing  HAN Jing-Tao
Affiliation:School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China
Abstract:Graphitized steel can have good machinability and formability, or high strength through controlling microstructure. The graphitization process is formation of graphite particles in graphitized steel, which is key to control the microstructure and properties of the steel. In this paper, the quenched high carbon steel with 0.66% carbon (mass fraction) was graphitized at 650, 680, and 710℃, respectively. The microstructure formed during the graphitization process was analyzed by a field emission scanning electron microscope, electron probe microanalysis, X-ray diffraction, and a transmission electron microscope. According to the dynamic theory of phase transformation, the kinetic curve of the graphitization process was drawn, and the corresponding kinetic equation was established. The results show that in the graphitization process, the quenched martensite is first transformed to the stable state of precipitation carbide. When the carbide is cementite Fe3C, the precipitation rate of graphite particles increases significantly. The acicular α-Fe in the matrix recrystallizes, and is gradually replaced by equiaxed ferrite. With prolonged graphitization time, the carbon content in ferrite decreases gradually; that is, it changes from a supersaturated state to a stable state. The carbon content increases to the peak value in graphite particles, whereas that of Fe decreases to the valley value. These changes show that the decomposed carbon of cementite, Fe3C, diffuses into the graphite core, whereas Fe diffuses from the graphite core, and then graphite particles are formed. Additionally, when steel is graphitized, the curve of graphite particle area fraction with time is an S shape; that is, the dynamic process of the tested steel is in accordance with the JMAK (Johnson-Mehl-Avrami-Kolmogorov) equation, and the value of n in the equation is between 1.5 and 1.7. 
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