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采用EBSD方法研究了TA15合金热挤压成形过程中的晶界特征分布演化规律.TA15合金分别在850、925和960℃温度下进行单筋正向热挤压变形,变形速率分别采用0.3mm/s和0.1mm/s,压下量分别取80%、60%、40%.研究表明,原始组织α相特殊晶界比例为12.04%,变形后特殊晶界比原始状态均有所减小.在变形温度为925℃,特殊晶界比例最小,960℃变形后特殊晶界比例有所升高;850℃和960℃变形后特殊晶界以∑5,∑17a和∑27a为主,而925℃变形后特殊晶界类型分布比较分散.随变形量的增加,特殊晶界数量先减小,后又增加,到变形量为60%时达到极大值;变形量40%和60%产生的特殊晶界以∑5,∑17a和∑27a类型为主,当变形量达到80%时,特殊晶界类型变得极为分散.随应变速率的增加,特殊晶界的比重减小,而小角晶界的比重增加.

参考文献

[1] 陈善华,吴杰,管登高,邹丛沛,邱绍宇.金属材料晶界工程研究进展[J].金属热处理,2006(03):1-6.
[2] Gupta G;Ampornrat P;Ren X;Sridharan K;Allen TR;Was GS .Role of grain boundary engineering in the SCC behavior of ferritic-martensitic alloy HT-9[J].Journal of Nuclear Materials: Materials Aspects of Fission and Fusion,2007(2/3):160-173.
[3] M. Michiuchi;H. Kokawa;Z.J. Wang .Twin-Induced grain boundary engineering for 316 austenitic stainless steel[J].Acta materialia,2006(19):5179-5184.
[4] G. Owen;V. Randle .On the role of iterative processing in grain boundary engineering[J].Scripta materialia,2006(10):959-962.
[5] Andre Luiz Pinto;Carlos Sergio da Costa Viana;Luiz Henrique de Almeida .Micromechanisms involved in grain boundary engineering of α-brass[J].Materials Science & Engineering, A. Structural Materials: Properties, Misrostructure and Processing,2007(1/2):14-19.
[6] 武保林.材料织构与晶界特征分布及其性能增强[J].沈阳航空工业学院学报,2002(03):1-6.
[7] 夏爽,周邦新,陈文觉,王卫国.高温退火过程中铅合金晶界特征分布的演化[J].金属学报,2006(02):129-133.
[8] XU Wen-chen;SHAN De-bin;LU Yan et al.Effects of hot deformation parameters on flow stress and establishment of constitutive relationship system of BT20 titanium alloy[J].Transactions of Nonferrous Metals Society of China,2005,15:167-168.
[9] Miaoquan Li;Hongsi Pan;Yingying Lin;Jiao Luo .High temperature deformation behavior of near alpha Ti-5.6Al-4.8Sn-2.0Zr alloy[J].Journal of Materials Processing Technology,2007(1):71-76.
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