scholarly journals Stacking Fault Energy and Deformation Twinning in Copper Crystals

1983 ◽  
Vol 47 (11) ◽  
pp. 903-911 ◽  
Author(s):  
Akitoshi Yamamoto ◽  
Nobutaka Narita ◽  
Jin-ichi Takamura ◽  
Hiroki Sakamoto ◽  
Naoto Matsuo
Keyword(s):  
Deformation Twinning ◽  
Stacking Fault ◽  
Stacking Fault Energy ◽  
Copper Crystals

Deformation twinning behaviors of the low stacking fault energy high-entropy alloy: An in-situ TEM study

2017 ◽  
Vol 137 ◽  
pp. 9-12 ◽  
Author(s):  
Jiabin Liu ◽  
Chenxu Chen ◽  
Yuqing Xu ◽  
Shiwei Wu ◽  
Gang Wang ◽  
...  
Keyword(s):  
Deformation Twinning ◽  
Stacking Fault ◽  
Stacking Fault Energy ◽  
High Entropy Alloy ◽  
In Situ Tem ◽  
High Entropy

Mechanical milling-induced deformation twinning in Fcc materials with high stacking fault energy

2003 ◽  
Vol 34 (3) ◽  
pp. 707-712 ◽  
Author(s):  
Jianhong He ◽  
Kyung H. Chung ◽  
Enrique J. Lavernia ◽  
Xiaozhou Liao ◽  
Yuntian T. Zhu
Keyword(s):  
Mechanical Milling ◽  
Deformation Twinning ◽  
Stacking Fault ◽  
Stacking Fault Energy ◽  
Fcc Materials

Deformation Textures of Ordered and Disordered Cu3Au*

1968 ◽  
Vol 12 ◽  
pp. 372-390 ◽  
Author(s):  
E. A. Starke ◽  
J. C. Ogle ◽  
C. J. Sparks
Keyword(s):  
Deformation Twinning ◽  
Stacking Fault ◽  
Stacking Fault Energy ◽  
Disordered Materials ◽  
Rolling Schedule ◽  
Total Reduction ◽  
Deformation Textures ◽  
Degree Of Order ◽  
Stacking Fault Energies

AbstractThe development of deformation textures of both initially disordered and ordered Cu3Au has been studied and discussed in terms of the stacking fault energies and twinning probabilities. No differences in the deforir.ation textures of the ordered and disordered materials were detected at deformations up to 40% reduction. However, at reductions of approximately 42% a marked difference was observed. This difference is attributed both to the degree of order and to the stacking fault energy of the ordered sample being conducive to deformation twinning at this stage of the rolling schedule. For samples which were reordered below the racrystallization temperature at intermediate stages of deformation (every 10% in total reduction) no differences between the ordered and initially disordered samples were observed up to 90% total reduction in thickness.

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