The Interplay of Convection, Conduction and Phase Transition in a Shape-Memory-Alloy

Author(s):  
Ingo Müller ◽  
Norbert Papenfuß-Janzen ◽  
Stefan Seelecke
Wear ◽  
2005 ◽  
Vol 259 (1-6) ◽  
pp. 309-318 ◽  
Author(s):  
Linmao Qian ◽  
Zhongrong Zhou ◽  
Qingping Sun

2013 ◽  
Vol 663 ◽  
pp. 397-402
Author(s):  
Bo Zhou ◽  
Tai Yue Yin ◽  
Shi Feng Xue

This paper focuses on the thermo-mechanical behaviors of the shape memory alloy board with a crack and under the torsion load. A stress field equation from mechanics of elasticity is used to describe the stress distribution around the crack tip in the shape memory alloy board. A martensitic phase transition equation is supposed to predict the martensitic phase transition behaviors of the field near the crack tip in the shape memory alloy board. The martensitic phase transition zones near the crack tip in the shape memory alloy board under the torsion load are numerically described based on the stress field equation and martensitic phase transition equation at various temperatures. Results show that the stress field equation and martensitic phase transition equation can predict the thermo-mechanical behaviors of the shape memory alloy board with a crack and under the torsion load effectively.


2010 ◽  
Vol 148-149 ◽  
pp. 1360-1363
Author(s):  
Yong Jun Wang ◽  
Zhen Qing Wang ◽  
Hong Qing Lv ◽  
Yu Long Wang

In order to investigate the performance of shape memory alloy wire, two types of alloy wire were studied. The results showed that the phase transition temperature of the superelastic wire were: Ms and Mf were 21.18 °C and 7.08 °C; As and Af were 12.32 °C and 25.13 °C. The phase transition temperature of memory effect alloy wire were that Ms =- 11.85 °C, Mf =- 29.37 °C, As = 36.77 °C, Af = 43.35 °C. By the tensile test of the SMA wire, the stress - strain curves of the two kinds of alloy wire were obtained.


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