High strength and high electrical conductivity bulk Cu

被引:95
作者
Han, K [1 ]
Walsh, RP
Ishmaku, A
Toplosky, V
Brandao, L
Embury, JD
机构
[1] Natl High Magnet Field Lab, Tallahassee, FL 32310 USA
[2] Inst Mil Engn, BR-22270290 Rio De Janeiro, Brazil
[3] McMaster Univ, Dept Mat Sci & Engn, Hamilton, ON, Canada
基金
美国国家科学基金会;
关键词
D O I
10.1080/14786430412331293496
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The achievement of both high strength and high electrical conductivity in bulk materials is challenging in the development of multifunctional materials, because the majority of the strengthening methods reduce the electrical conductivity of the materials significantly. At room temperature, dislocations have little scattering effect on conduction electrons. Thus, a high density of dislocations can strengthen conductors without significantly increasing the resistivity. However, at room temperature (RT), which is defined as 295 +/- 2K in this paper, deformation can only introduce a limited number of dislocations in pure metals due to dislocation annihilation, i.e. recovery. This limitation is expanded by a well-controlled liquid nitrogen temperature (LNT), which is defined as 77 +/- 0.5 K in this paper, deformation process that permits accumulation of both nanotwins and a high density of dislocations accompanied by significantly less recovery than that in RT-deformed samples. The dislocations are organized, into refined dislocation cells, with thicker cell boundaries in LNT-deformed samples than those deformed at RT. LNT deformation stores more energy in the material than RT deformation. LNT deformation produces bulk pure Cu with a yield strength about 1.5 times that of RT-deformed Cu. The RT resistivity increase is less than 5% compared with that of annealed Cu.
引用
收藏
页码:3705 / 3716
页数:12
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