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Microstructure of Hot Rolled 1.0C-1.5Cr Bearing Steel and Subsequent Spheroidization Annealing

机译:1.0C-1.5Cr热轧轴承钢的组织及随后的球化退火

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The effect of final rolling temperature and cooling process on the microstructure of 1.0C-1.5Cr bearing steel was studied, and the relationship between the microstructure parameters and subsequent spheroidization annealing was analyzed. The results indicate that the increase of water-cooling rate after hot rolling and the decrease of final cooling temperature are beneficial to reducing both the pearlite interlamellar spacing and pearlite colony size. Prior austenite grain size can be reduced by decreasing the final rolling temperature and increasing the water-cooling rate. When the final rolling temperature was controlled around 1103 K (830 A degrees C), the subsequent cooling rate was set to 10 K/s and final cooling temperature was 953 K (680 A degrees C), the precipitation of grain boundary cementite was suppressed effectively and lots of rod-like cementite particles were observed in the microstructure. Interrupted quenching was employed to study the dissolution behavior of cementite during the austenitizing at 1073 K (800 A degrees C). The decrease of both pearlite interlamellar spacing and pearlite colony size could facilitate the initial dissolution and fragmentation of cementite lamellae, which could shorten the spheroidization time. The fragmentation of grain boundary cementite tends to form large-size undissolved cementite particles. With the increase of austenitizing time from 20 to 300 minutes, mean diameter of undissolved cementite particles increases, indicating the cementite particle coarsening and cementite dissolution occuring simultaneously. Mean diameter of cementite particles in the final spheroidized microstructure is proportional to the mean diameter of undissolved cementite particles formed during partial austenitizing.
机译:研究了终轧温度和冷却工艺对1.0C-1.5Cr轴承钢组织的影响,分析了组织参数与随后球化退火之间的关系。结果表明,热轧后水冷速度的增加和最终冷却温度的降低有利于减小珠光体的层间间距和珠光体的菌落尺寸。可通过降低最终轧制温度并提高水冷速率来降低先前的奥氏体晶粒尺寸。将最终轧制温度控制在1103K(830A℃)左右时,将其后的冷却速度设定为10K / s,将最终冷却温度设为953K(680A℃),可以抑制晶界渗碳体的析出。有效地观察到了许多棒状渗碳体颗粒。采用间断淬火研究渗碳体在1073 K(800 A℃)下奥氏体化过程中的溶解行为。珠光体层间间距的减小和珠光体菌落尺寸的减小均可促进渗碳体片层的初始溶解和破碎,从而缩短球化时间。晶界渗碳体的破碎易于形成大尺寸的不溶渗碳体颗粒。随着奥氏体化时间从20分钟增加到300分钟,未溶解渗碳体颗粒的平均直径增加,表明渗碳体颗粒变粗和渗碳体溶解同时发生。最终球化微结构中渗碳体颗粒的平均直径与部分奥氏体化过程中形成的未溶解渗碳体颗粒的平均直径成比例。

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