Anelastic relaxation behavior of hydrogen in L12 ordered intermetallic compound Ni3Al

2002 ◽  
Vol 47 (9) ◽  
pp. 625-629 ◽  
Author(s):  
C.B. Jiang ◽  
H. Li ◽  
C.X. Huang ◽  
G.Y. Li ◽  
S.D. Wu ◽  
...  
Author(s):  
S. M. L. Sastry

Ti3Al is an ordered intermetallic compound having the DO19-type superlattice structure. The compound exhibits very limited ductility in tension below 700°C because of a pronounced planarity of slip and the absence of a sufficient number of independent slip systems. Significant differences in slip behavior in the compound as a result of differences in strain rate and mode of deformation are reported here.Figure 1 is a comparison of dislocation substructures in polycrystalline Ti3Al specimens deformed in tension, creep, and fatigue. Slip activity on both the basal and prism planes is observed for each mode of deformation. The dominant slip vector in unidirectional deformation is the a-type (b) = <1120>) (Fig. la). The dislocations are straight, occur for the most part in a screw orientation, and are arranged in planar bands. In contrast, the dislocation distribution in specimens crept at 700°C (Fig. lb) is characterized by a much reduced planarity of slip, a tangled dislocation arrangement instead of planar bands, and an increased incidence of nonbasal slip vectors.


2005 ◽  
Vol 86 (12) ◽  
pp. 121908 ◽  
Author(s):  
E. Partyka ◽  
W. Sprengel ◽  
H. Weigand ◽  
H.-E. Schaefer ◽  
F. Krogh ◽  
...  

2008 ◽  
Vol 458 (1-2) ◽  
pp. 277-281 ◽  
Author(s):  
Yongzhang Huang ◽  
Wenxia Yuan ◽  
Zhiyu Qiao ◽  
Olga Semenova ◽  
Gabriel Bester ◽  
...  

1993 ◽  
Vol 170 (1-2) ◽  
pp. 11-18 ◽  
Author(s):  
J.M. Brzeski ◽  
J.E. Hack ◽  
R. Darolia ◽  
R.D. Field

1990 ◽  
Vol 201 ◽  
Author(s):  
Michael J. Sabochick ◽  
Nghi Q. Lam

AbstractAmorphization of the B2 intermetallic compound NiTi under electron irradiation has been investigated using molecular dynamics. The effect of irradiation was simulated using two processes: 1) Ni and Ti atoms were exchanged, resulting in chemical disorder, and 2) Frenkel pairs were introduced, leading to the formation of stable point defects and also chemical disorder upon mutual recombination of interstitials and vacancies. After ∼0.1 exchanges per atom, the first process resulted in an energy increase of approximately 0.11 eV/atom and a volume increase of 1.91%. On the other hand, after introducing ∼0.5 Frenkel pairs per atom, the second process led to smaller increases of 0.092 eV/atom in energy and 1.43% in volume. The calculated radial distribution functions (RDFs) were essentially identical to each other and to the calculated RDF of a quenched liquid. The structure factor, however, showed that long-range order was still present after atom exchanges, while the introduction of Frenkel pairs resulted in the loss of long-range order. It was concluded that point defects are necessary for amorphization to occur in NiTi, although chemical disorder alone is capable of storing enough energy to make the transition possible.


1995 ◽  
Vol 3 (1) ◽  
pp. 47-56 ◽  
Author(s):  
M.-X. Zhang ◽  
K.-C. Hsieh ◽  
Y.A. Chang ◽  
J.P. Neumann ◽  
A.D. Romig

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