The effects of second-alloying-element on the formability of Mg-Sn alloys in respect of the stacking fault energies of slip systems

2021 ◽  
Vol 29 ◽  
pp. 102829
Author(s):  
Xiongying Cheng ◽  
Yuan Yuan ◽  
Tao Chen ◽  
Zebang Zheng ◽  
Lifeng Ma ◽  
...  
RSC Advances ◽  
2015 ◽  
Vol 5 (95) ◽  
pp. 77831-77838 ◽  
Author(s):  
Tao Fu ◽  
Xianghe Peng ◽  
Yinbo Zhao ◽  
Rong Sun ◽  
Deqiang Yin ◽  
...  

We calculate the generalized stacking fault energies along different slip directions in various slip planes of VN and found that the 〈110〉 directions show the lowest maximum stacking fault energies.


2019 ◽  
Vol 55 (2) ◽  
pp. 271-282
Author(s):  
M. Muzyk ◽  
K.J. Kurzydłowski

Generalised stacking fault energies of copper alloys have been calculated using density functional theory. Stacking fault energy of copper alloys is correlated with the d?electrons number of transition metal alloying element. The tendency to twiningis also modified by the presence of alloying element in the deformation plane. The results suggest that Cu ?transition metal alloys with such elements as Cr, Mo, W, Mn, Re are expected to exhibit great work hardening rate due to the tendency to emission of the partial dislocations.


2020 ◽  
Vol 35 (20) ◽  
pp. 2718-2725
Author(s):  
Gengsen Xu ◽  
Xiaoyu Chong ◽  
Yunxuan Zhou ◽  
Yan Wei ◽  
Changyi Hu ◽  
...  

Abstract


2012 ◽  
Vol 24 (50) ◽  
pp. 505403 ◽  
Author(s):  
S L Shang ◽  
C L Zacherl ◽  
H Z Fang ◽  
Y Wang ◽  
Y Du ◽  
...  

1993 ◽  
Vol 67 (6) ◽  
pp. 1447-1457 ◽  
Author(s):  
S. Crampin ◽  
D. D. Vvedensky ◽  
R. Monnier

1972 ◽  
Vol 9 (2) ◽  
pp. 581-591
Author(s):  
E. Torfs ◽  
R. de Ridder ◽  
J. van Landuyt ◽  
S. Amelinckx

1967 ◽  
Vol 45 (2) ◽  
pp. 1235-1249 ◽  
Author(s):  
F. W. J. Pargeter ◽  
M. B. Ives

Polycrystalline specimens of α-phase copper–aluminium alloys of varying composition, amalgamated with mercury, have been deformed in tension in a soft tensile machine. In all cases, brittle intergranular failure occurred at stresses and strains below those required for fracture in air, the degree of embrittlement increasing with increasing aluminium content. The alloys having stacking-fault energies less than '~8 erg/cm2 were found to obey quite well the Petch–Stroh relation:[Formula: see text]The other alloys showed deviations from this relation which became more marked with increasing stacking-fault energy. Values of the fracture energy, varying from ~48 erg/cm2 for pure copper to ~470 erg/cm2 for Cu −8 wt.% Al, have been obtained for all of the alloys. These values are only applicable for relatively small grain sizes.The deviation from the Petch–Stroh relation in the high stacking-fault energy alloys is thought to be due to their tendency to show cross-slip and cellular-network formation, rather than coplanar arrays of dislocations as required by the Stroh model. The low stacking-fault energy alloys typically show well-defined pileups and so obey the Petch–Stroh relations, as expected.


2015 ◽  
Vol 817 ◽  
pp. 706-711
Author(s):  
Yu Fei Shao ◽  
Xin Yang ◽  
Jiu Hui Li ◽  
Xing Zhao

Indenter size effect on the reversible incipient plasticity of Al (001) surface is studied by quasicontinuum simulations. Two cylindrical indenters with the radii 2.5nm and 17.5nm are used to penetrate the surface respectively, in displacement-control in steps of 0.02 nm. Results show that the plasticity under the small indenter is reversible, since it is dominated by the nucleation of a thin deformation twin, which can be fully removed after withdrawal of the indenter, due to the imaging force and stacking fault energy. Under the large indenter, multiple slip systems are activated simultaneously when incipient plasticity occurs, a few twin, dislocation and stacking fault ribbons still remain under the surface when the indenter has been completely retracted, thus the plasticity is irreversible.


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