Preliminary Investigations of a High Temperature Cu-13.3%Al-4%Ni Shape Memory Alloy Single Crystal

Author(s):  
Steve Trigwell ◽  
Ganesh Kumara K. ◽  
Abhijit Bhattacharyya ◽  
Muhammed A. Qidwai

Preliminary investigations on the constitutive response of a Cu-13.3%Al-4%Ni (wt%) shape memory alloy single crystal with stress-free transformation temperatures around 100 to 150°C are reported. Room temperature stress cycling tests were carried out at very low deformation rates. Reproducible stress/strain curves of up to 9% strain due to detwinning (martensitematensite phase transformations) with no plastic deformation were obtained. The data also indicated that a period of stress cycling is required to stabilize the material before reproducible stress-strain curves are obtained due to martensite reorientation.

1994 ◽  
Author(s):  
Pyoung-Kil Yoo ◽  
G.-S. Ieen ◽  
Hyo-Yeol Park ◽  
Seok-Kil Han ◽  
Min-Su Jang

2018 ◽  
Vol 144 ◽  
pp. 748-757 ◽  
Author(s):  
Harshad M. Paranjape ◽  
Partha P. Paul ◽  
Behnam Amin-Ahmadi ◽  
Hemant Sharma ◽  
Darren Dale ◽  
...  

Materia Japan ◽  
2019 ◽  
Vol 58 (3) ◽  
pp. 137-143
Author(s):  
Toshihiro Omori ◽  
Tomoe Kusama ◽  
Sumio Kise ◽  
Toyonobu Tanaka ◽  
Yoshikazu Araki ◽  
...  

2006 ◽  
Vol 13-14 ◽  
pp. 305-312
Author(s):  
Kenichi Yoshida ◽  
T. Yasuda ◽  
D. Tani ◽  
H. Nishino

Dynamic behavior of two types of martensitic transformations during tensile deformation of Cu-Al-Ni shape memory alloy single crystal has been investigated using an acoustic emission waveform analysis. Two kinds of martensitic transformations consist of β1 ⇔ β1′ (structural change of DO3 to 18R) and β1 ⇒ γ1′ (structural change of DO3 to 2H), each of which is called super-elastic and thermo-elastic martensitic transformations, respectively. These two types of martensitic transformations could be obtained during tensile deformation because of different heat treatment. The rise time at the source (the source rise time) in finite elastic solid by the modified Takashima’s method was analyzed using the acoustic emission waveform detected during the martensitic transformation. The mean source rise time to the γ1′ phase was smaller than that to the β1′ phase before yielding and became the same after yielding. The former result means that the nucleation of the γ1′ phase is faster than that of the β1′ phase because of different crystallographic structure. The latter result is that the growth rate of the γ1′ phase is the same as that of the β1′ phase.


Author(s):  
В.И. Николаев ◽  
А.В. Солдатов ◽  
Р.Б. Тимашов ◽  
В.М. Крымов

Stress-strain behavior of a cubic-shaped Ni49Fe18Ga27Co6 shape memory single crystal uniaxially compressed in three directions perpendicular to its faces was studied. The crystallographic orientation of the sample was chosen so that the sample was deformed along two <110>А and one [001]А directions. A fundamentally different stress-strain behavior was observed for the deformations along <110>A and [001]A directions. At room temperature, irrespective of the magnitude of the phase strain, the crystal compressed in [001]A exhibited superelastic behavior i.e. the strain fully recovered after unloading. In contrast, deformation along <110>A directions to the strain levels above 4% induced a residual shape memory strain after the unloading. Strains measured along the directions perpendicular to the compression axis indicate an anomalous behavior of the Poisson's ratio.


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