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研究了退火时间对超快速加热连续退火工艺下V微合金化低Si含P系热镀锌用TRIP钢显微组织特征与力学性能的影响.结果表明,超快速连续退火过程中,高密度位错以及细小、弥散的v(C,N)分布于基体中,大部分析出粒子直径在4-10 nm之间.残余奥氏体体积分数随着退火时间的延长而增加,但其形貌特征发生改变,随着退火时间延长到90 s时,以厚度在80-120 nm之间的片层状残余奥氏体为主;继续延长到180 s时,残余奥氏体的片层厚度增加至200-600 nm,趋于块状.随着退火时间的延长,拉伸强度逐渐降低,而延伸率和加工硬化指数呈上升趋势;表征强度与塑性综合性能的强塑积由退火时间t=10 s时的23976MPa.%降低到t=180 s时的23625MPa.%.

参考文献

[1] Yi H L,Lee K Y,Bhadeshia H K D H.Mater Sci Eng,2011; A528:5900
[2] Mazzoni-Leduc L,Pardoen T,Massart T J.Eur J Mechanics,2010; 29A:132
[3] Ding H,Ding H,Song D,Tang Z Y,Yang P.Mater Sci Eng,2011; A528:868
[4] Jimenez Melero E,Dijk N H,Zhao L,Sietsma J,Offerman S E,Wright J P,Zwaag S.Acta Mater,2009; 57:533
[5] Herrera C,Ponge D,Raabe D.Acta Mater,2011; 59:4653
[6] Jacques P J,Girault E,Mertens A,Verlinden B,van Humbeeck J,Delannay F.ISIJ Int,2001; 41:1068
[7] Hojo T,Sugimoto K I,Mukai Y,Ikeda S.ISIJ Int,2008;48:824
[8] Mahieu J,Maki J,De Cooman B C,Claessens S.Metall Mater Trans,2002; 33A:2573
[9] De Cooman B C.Current Opinion Solid State Mater Sci,2004; 8:285
[10] Sakuma Y,Matsumura O,Akisue O.ISIJ Int,1991; 31:1348
[11] Basuki A,Aernoudt E.Scr Mater,1999; 40:1003
[12] Balk S C,Kim S,Jin Y S,Kwon O.ISIJ Int,2001; 41:290
[13] Kim S J,Lee C G,Lee T H,Oh C S.ISIJ Int,2002; 42:1452
[14] Pereloma E V,Russell K F,Miller M K,Timokhina I B.Scr Mater,2008; 58:1078
[15] Pereloma E V,Timokhina I B,Hodgson P D.Mater Sci Eng,1999; A273-275:448
[16] Jiao S,Hassani F,Donaberger R L,Essadiqi E,Yue S.ISIJ Int,2002; 42:299
[17] Chen H C,Era H,Shimizu M.Metall Trans,1989; 20A:437
[18] Lesch C,Alvarez P,Bleck W,Gil Sevillano J.Metall Mater Trans,2007; 38A:1882
[19] Salvatori I,Moore W B R.ISIJ Int,2000; 40(suppl 1):179
[20] Muljono D,Ferry M,Dunne D P.Mater Sci Eng,2001;A303:90
[21] Ray R K,Jonas J J,Hook R E.Int Mater Rev,1994; 39:129
[22] Chowdhury S G,Pereloma E V,Santos D B.Mater Sci Eng,2008; A480:540
[23] Funakawa Y,Shiozaki T,Tomita K,Yamamoto T,Maeda E.ISIJ Int,2004; 44:1945
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