利用SEM和TEM原位拉伸方法研究了轧后冷却制度对X80级抗大变形管线钢组织的影响及低屈强比的微观机理.结果表明:采用轧后弛豫+控制冷却的工艺可以获得铁索体+贝氏体双相组织,弛豫终止温度是影响铁素体体积含量和晶粒大小的决定因素.当弛豫终止温度区间为690-705℃时,试样的强度和塑性达到了较好的匹配,满足X80级抗大变形管线钢的性能要求.弛豫终止温度越低,铁素体体积含量越高,晶粒尺寸越大,屈强比越低.对拉伸过程进行动态原位观察的结果表明,铁索体(软相)和贝氏体(硬相)的协调变形机制是屈强比降低的原因.
参考文献
[1] | Li H L,Li X,Ji L K.Weld Pipe Tube,2007; 30(5):6 (李鹤林,李霄,吉玲康.焊管,2007;30(5):6) |
[2] | Mohr W.Strain-based Design of Pipelines.Washinton:EWI,2003:10 |
[3] | Ishikawa N,Parks D M,Socrate S,Kurihara M.ISIJ Int,2000; 40:1170 |
[4] | Shen X P,Lei T Q,Liu J Z.Acta Metall Sin,1987; 23:151(沈显璞,雷廷权,刘剑壮.金属学报,1987;23:151) |
[5] | Li L,Ding H,Wen J L,Song H M,Zhang P J.Chin J Mater Res,2007; 21:519(李龙,丁桦,温景林,宋红梅,张丕军.材料研究学报,2007;21:519) |
[6] | Han B Q,Su Y.J Mater Proc Technol,2003; 136:102 |
[7] | Tomotam Y,Umemoto I,Komatsubara O,Hiramatsu A,Nakajima N.ISIJ Int,1992; 32:343 |
[8] | Endo S,Kurihara M,Suzuki N.Mater Jpn,2000; 39:167 |
[9] | Ishikawa N,Endo S,Kondo J.JFE Technol Report,2006;7:20 |
[10] | KIM Y M,KIM S K,LIM Y J.ISIJ Int,2002; 42:1574 |
[11] | Shikana N,Kagawa H,Kuriha M.ISIJ Int,1992; 32:337 |
[12] | Huper T,Endo S,Ishikawa N.ISIJ Int,1999; 39:288 |
[13] | Yu Q B,Zhao X P,Sun B.Iron Steel,2007; 42:76(于庆波,赵贤平,孙斌.钢铁,2007;42:76) |
[14] | Ma M T,Wu B R.Dual Phase Steel-Physics and Mechanical Metallurgy,Beijing:Metallurgical Industry Press,1988:72(马鸣图,吴宝榕.双相钢-物理和力学冶金.北京:冶金工业出版社,1988:72) |
[15] | Li S X,Cui G R.J App Phy,2007; 101:083525-1 |
[16] | Tang Z H,Waldo S.Mater Sci Eng,2008; A408:402 |
[17] | Li H L,Guo S W,Feng Y R,Huo C Y,Chai H F.Microstructure Analysis and Metallograph Identification of High-strength Microalloying Pipelines Steel.Beijing:Petroleum Industry Press,2001:8(李鹤林,郭生武,冯耀荣,霍春勇,柴惠芬.高强度微合金管线钢显微组织分析与鉴别图谱.北京:石油工业出版社,2001:8) |
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