Comparison of TEM Observations with Dislocation Core Structure Calcuiations in B2 Ordered Compounds

1990 ◽  
Vol 213 ◽  
Author(s):  
D. Farkas ◽  
R. Pasianot ◽  
E. J. Savino ◽  
D.B. Miracle

ABSTRACTDislocation core structures have been calculated using atomistic computer simulations in NiAl and other B2 compounds. In the present work the calculated dislocation core structure are correlated with the known deforniatiorn behavior of B2 alloys. It is found that for the high ordering energy compounds <111> dislocations do not split in the simulations, in agreement with the experimental observations. It is also found that core structures for certain <111> and 1/2 <111> dislocations are spread in { 112} planes, which is consistent with the slip plane often reported for these dislocations. For the < 100> dislocations several orientations of the dislocation line produce sessile core configurations, whereas other orientations produce relatively more glissile cores. However, a structural transition of each of these dislocation cores may be required before < 100> dislocations become mobile, and this is consistent with the limited tensile ductility observed in NiAl “soft” single crystals below 200°C. Core structure simulations for < 110> dislocations are also reported and are discussed with respect to the importance of these dislocations in the deformation of NiAl.

2019 ◽  
Vol 10 (1) ◽  
Author(s):  
D. L. Medlin ◽  
N. Yang ◽  
C. D. Spataru ◽  
L. M. Hale ◽  
Y. Mishin

2012 ◽  
Vol 606 (21-22) ◽  
pp. 1728-1738 ◽  
Author(s):  
Lixin Zhang ◽  
W.E. McMahon ◽  
Y. Liu ◽  
Y. Cai ◽  
M.H. Xie ◽  
...  

1988 ◽  
Vol 133 ◽  
Author(s):  
S. E. Hsu ◽  
C. H. Tong ◽  
T. S. Lee ◽  
T. S. Liu

ABSTRACTNi-Al-Cr single crystals with 4 at% Cr and different levels of aluminum content are grown in a directional solidification facility. The crystals are creep tested at temperatures from 760°C to 860°C. Steady state, as well as transient, creep rates are measured. The results show that Cr modified Ni3 A1, when tested along the <100> direction, exhibit remarkably high values of activation energy for creep. Along with evidence from dislocation structures, it is likely that there is a change in the dislocation core structure upon Cr addition.


1992 ◽  
Vol 291 ◽  
Author(s):  
Roberto Pasianot ◽  
Eduardo J. Savino ◽  
Zhao-Yang Xie ◽  
Diana Farkas

ABSTRACTFlexible boundary codes for the atomistic simulation of dislocations and other defects have been developed in the past mainly by Sinclair [1], Gehlen et al.[2], and Sinclair et al.[3]. These codes permitted the use of smaller atomic arrays than rigid boundary codes, gave descriptions of core non-linear effects and allowed fair assessments of the Peierls stress for dislocation motion. Green functions (continuum or discrete) or surface traction forces were used to relax the boundary atoms.A much simpler approach is followed here. Core and mobility effects at the boundary are accounted for by a dipole tensor centered at the dislocation line, whose components constitute six more parameters of the minimization process. Results are presented for [100] dislocations in NiAl. It is shown that, within the limitations of the technique, reliable values of the Peierls stress are obtained.


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