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采用轴向拉应力、周向压应力的方式对工业纯钛进行室温加工,研究不同加工变形量下孪晶组织和力学性能的演化规律,并通过变形样品退火后的组织与硬度变化表征孪晶的稳定性.结果表明:孪晶数量和尺寸与加工变形量呈线性变化,60%变形量样品中出现加工流线并达到塑性极大值;550℃退火出现再结晶晶粒,形变孪晶550℃以下可短时亚稳存在.

参考文献

[1] S. NEMAT-NASSER;W. G. GUO;J. Y. CHENG .MECHANICAL PROPERTIES AND DEFORMATION MECHANISMS OF A COMMERCIALLY PURE TITANIUM[J].Acta materialia,1999(13):3705-3720.
[2] 段晓鸽,江海涛,刘继雄,毕艳君.工业纯钛TA2冷轧板再结晶过程的研究[J].稀有金属,2012(03):353-356.
[3] M. BATTAINI;E.V. PERELOMA;C.H.J. DAVIES .Orientation Effect on Mechanical Properties of Commercially Pure Titanium at Room Temperature[J].Metallurgical and Materials Transactions, A. Physical Metallurgy and Materials Science,2007(2):276-285.
[4] Terada D;Inoue S;Tsuji N .Microstructure and mechanical properties of commercial purity titanium severely deformed by ARB process[J].Journal of Materials Science,2007(5):1673-1681.
[5] 刘清华,惠松骁,叶文君,王国,胡光山.不同组织状态TC4ELI钛合金动态力学性能研究[J].稀有金属,2012(04):517-522.
[6] Lei Bao;Christophe Schuman;Jean-Sebastien Lecomte;Marie-Jeanne Philippe;Xiang Zhao;Claude Esling .A Study of Twin Variant Selection and Twin Growth in Titanium[J].Advanced Engineering Materials,2011(10):928-932.
[7] Ayman A. Salem;Surya R. Kalidindi;Roger D. Doherty .Strain hardening regimes and microstructure evolution during large strain compression of high purity titanium[J].Scripta materialia,2002(6):419-423.
[8] I. Kim;J. Kim;D. H. Shin;X. Z. Liao;Y. T. Zhu .Deformation twins in pure titanium processed by equal channel angular pressing[J].Scripta materialia,2003(6):813-817.
[9] 王成,赵西成,杨西荣,王幸运.室温ECAP变形工业纯钛的微观组织研究[J].热加工工艺,2009(14):1-3.
[10] 付文杰,赵西成,杨西荣,郑艳霞.室温等径弯曲通道变形工业纯钛的组织及性能研究[J].热加工工艺,2007(18):21-23,61.
[11] SUN Qiao-yan,SONG Xi-ping,GU Hai-cheng.Twinning induced plasticity in commercially pure titanium at low temperature[J].中国有色金属学会会刊(英文版),2001(01):132-134.
[12] 毛萍莉,刘正,王长义,王峰.高应变速率下AZ31镁合金的各向异性及拉压不对称性[J].中国有色金属学报(英文版),2012(05):1262-1269.
[13] 卢磊,卢柯.纳米孪晶金属材料[J].金属学报,2010(11):1422-1427.
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