利用Hopkinson杆,采用动态压缩实验研究帽形样品的工业纯钛在高应变率(103 s-1)下的变形与失效机制.从时间-剪应力曲线分析材料的剪切变化规律.结果表明:轧制变形后的试样,它的绝热剪切敏感性明显变强;而在轧制变形量相同的情况下,从材料厚度方向上取的试样,其绝热剪切敏感性比其它方向强.通过光学显微镜、扫描电镜和透射电镜分析其显微组织的变化规律.结果表明:试样的受剪部位均可观察到明显的绝热剪切带.绝热剪切带是材料宏观失效的先兆,带内晶粒细小,为等轴晶,发生了再结晶,带中的微裂纹、微空洞的形成最终导致材料失效.
参考文献
[1] | Ni J G;Tao C H;Li S N.A course on damage mechanics[M].北京:科学出版社,1997:1. |
[2] | Meyers M A.Dynamic behavior of materials[M].New York:John Wiley and Sons,Inc,1994 |
[3] | Bai Yi long .Adiabatic shear banding[J].Res Mechanics,1990,31:133-203. |
[4] | Grady D E .Dissipation in adiabatic shear bands[J].Mechanics of Materilas,1994,17(03):289-293. |
[5] | Culver R S.Metall effects at high strain rates[M].New York:Plenum Press,1973:519-575. |
[6] | Harding J.Materials at high strain rates[M].New York:Elsevier Applied Science,1987:133. |
[7] | Bai Y;Dodd B.Adiabatic shear Localization[M].Oxford:Pergam on,1992:1-7. |
[8] | Hines J A;Vecchio K S;Ahzi S .A model for microstructure evolution in adiabatic shear bands[J].Metallurgical and Materials Transactions A:Physical Metallurgy and Materials Science,1998,29A:191-203. |
[9] | Yu J L;Dong X L;Zhang J Y .A study of adiabatic shear plugging in Ti6A14V alloy[J].Key Engineering Materials,2000,177-180:387-392. |
[10] | Blazynski T Z.Materials at high strain rates[M].London and New York:Elsevier Applied Science,1987:133. |
[11] | 佟景伟;乌时毅;李鸿琦 .高应变率拉伸SHB试验设备的研制和测试技术[J].力学学报,1994,26:99-103. |
[12] | 李强;徐永波;赖祖涵 .Monel合金高速塑性剪切变形与动态重结晶[J].金属学报,1999,35:49-52. |
[13] | Wright T W;Walter J W .On stress collapse in adiabatic shear bands[J].Journal of the Mechanics and Physics of Solids,1987,35:701-720. |
[14] | Cho K M;Lee S .Adiabatic shear band formation during dynamic torsional deformation of an HY 100 steel[J].ACTA METALLURGICA ET MATERIALIA,1993,41:923-932. |
[15] | Cahn R W.Recrystallization of mtallic[M].Stuttgart:Riederer,1971:43. |
[16] | 刘新芹,王富耻,王琳,路永胜.钢中绝热剪切带的动态损伤演化[J].兵器材料科学与工程,2004(03):17-21. |
[17] | 侯增寿;卢光熙.金属学原理[M].上海:上海科学技术出版社,1990:175-195. |
上一张
下一张
上一张
下一张
计量
- 下载量()
- 访问量()
文章评分
- 您的评分:
-
10%
-
20%
-
30%
-
40%
-
50%