High temperature shape memory behavior of Ni50.3Ti25Hf24.7 single crystals

2016 ◽  
Vol 115 ◽  
pp. 133-136 ◽  
Author(s):  
L. Patriarca ◽  
Y. Wu ◽  
Huseyin Sehitoglu ◽  
Y.I. Chumlyakov
2011 ◽  
Vol 65 (7) ◽  
pp. 577-580 ◽  
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H.E. Karaca ◽  
S.M. Saghaian ◽  
B. Basaran ◽  
G.S. Bigelow ◽  
R.D. Noebe ◽  
...  

2015 ◽  
Vol 87 ◽  
pp. 128-141 ◽  
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H.E. Karaca ◽  
H. Tobe ◽  
M. Souri ◽  
R. Noebe ◽  
...  

2009 ◽  
Vol 107 (2) ◽  
pp. 194-205 ◽  
Author(s):  
Yu. I. Chumlyakov ◽  
E. Yu. Panchenko ◽  
A. V. Ovsyannikov ◽  
S. A. Chusov ◽  
V. A. Kirillov ◽  
...  

2017 ◽  
Vol 50 (10) ◽  
pp. 3903-3910 ◽  
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Qingbao Guan ◽  
Stephen J. Picken ◽  
Sergei S. Sheiko ◽  
Theo J. Dingemans

2006 ◽  
Vol 515 (4) ◽  
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Mohanchandra K. Panduranga ◽  
Daniel D. Shin ◽  
Gregory P. Carman

2009 ◽  
Vol 57 (4) ◽  
pp. 1068-1077 ◽  
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Pio John S. Buenconsejo ◽  
Hee Young Kim ◽  
Hideki Hosoda ◽  
Shuichi Miyazaki

1996 ◽  
Vol 459 ◽  
Author(s):  
Yu.I. Chumlyakov ◽  
I. V. Kireeva ◽  
Yu.I. Zuev ◽  
A. G. Lyisyuk

ABSTRACTThe dependence of shape memory effect (SME) and pseudoelasticity (PE) on crystal orientation and on sign of applied stresses (tension/compression) has been investigated on Ti-40%Ni-10%Cu (at.%) single crystals. It have been shown that both SME and PE depend on an orientation and an applied stress sign. Asymmetry effects were found at deformation in high-temperature B2 phase and in the range of stress-induced martensite transformations.


2013 ◽  
Vol 738-739 ◽  
pp. 82-86 ◽  
Author(s):  
Thomas Niendorf ◽  
Jayaram Dadda ◽  
Jan Lackmann ◽  
James A. Monroe ◽  
Ibrahim Karaman ◽  
...  

This paper reports on the tension-compression asymmetry of [001]-oriented Co49Ni21Ga30 single crystals at elevated temperatures. Maximum strains of -4.8 % and 8.6 % in compression and tension, respectively, were found. A linear Clausius-Clapeyron relationship was observed for both stress-states where the smaller slope in tension resulted in a significant increase of the phase transformation temperatures with stress, which reached 180 °C under a constant stress level of 150 MPa. In addition, the material demonstrated a large pseudoelastic temperature range of about 300 °C under both stress state conditions. The results in this study unequivocally indicate the potential of these alloys for applications where elevated temperatures and stress levels prevail.


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