Temperature dependence of thermoelectric power and thermal conductivity in ferromagnetic shape memory alloyNi50Mn34In16in magnetic fields

2010 ◽  
Vol 81 (19) ◽  
Author(s):  
L. S. Sharath Chandra ◽  
M. K. Chattopadhyay ◽  
V. K. Sharma ◽  
S. B. Roy ◽  
Sudhir K. Pandey
2018 ◽  
Vol 741 ◽  
pp. 689-692
Author(s):  
V. Khovaylo ◽  
I. Tereshina ◽  
G. Politova ◽  
A. Karpenkov ◽  
S. Taskaev ◽  
...  

Materials ◽  
2014 ◽  
Vol 7 (5) ◽  
pp. 3715-3734 ◽  
Author(s):  
Takuo Sakon ◽  
Kohei Otsuka ◽  
Junpei Matsubayashi ◽  
Yuushi Watanabe ◽  
Hironori Nishihara ◽  
...  

Aerospace ◽  
2003 ◽  
Author(s):  
LeAnn E. Faidley ◽  
Marcelo J. Dapino ◽  
Gregory N. Washington ◽  
Thomas A. Lograsso

Recent work on ferromagnetic shape memory nickel-manganese-gallium (Ni-Mn-Ga) has demonstrated several characteristics which make this material attractive as an active element for the next generation of intelligent transducers. Alloys of martensitic Ni-Mn-Ga can strain up to 6% as a result of the rotation of twin variants and associated twin boundary motion which occur in these materials in response to magnetic fields. The magnetic actuation holds promise in transducer design because it can lead to enhanced frequency response compared with shape memory alloys with comparable strains. In this paper, we report on experimental measurements collected from a Ni50Mn28.7Ga21.3 sample which has been tested in a solenoid transducer by means of a novel drive configuration consisting of a collinear uniaxial field-uniaxial stress pair. We have observed that the elastic modulus of a Ni-Mn-Ga sample driven in these conditions changes substantially in response to varying bias field. In this paper, we further investigate the dependence of the elastic modulus on ac field intensity and mechanical load as well as bias field. Quasistatic, white noise, and swept-sine excitations were employed to examine the behavior of Ni50Mn28.7Ga21.3 driven under various combinations of magnetic fields and mechanical loads. Mechanically free quasi-static tests demonstrate reversible strains of 6300 με which are consistent with prior measurements on samples with similar composition near the Heusler stoichiometry. Dynamic measurements reveal a significant stiffness increase, of up to 209%, with dc bias field. This frequency shift or ΔE effect is shown to originate in the Ni-Mn-Ga sample and is believed to stem from the reorientation of twin variants in response to varying dc field. These results might facilitate a new class of solenoid-based Ni-Mn-Ga transducers for tunable vibration absorber applications, and lay the ground work for developing methods and criteria for the implementation of broadband Ni-Mn-Ga transducer technologies.


Materials ◽  
2020 ◽  
Vol 13 (13) ◽  
pp. 2906
Author(s):  
Amadeusz Łaszcz ◽  
Mariusz Hasiak ◽  
Jerzy Kaleta

The temperature dependence of magnetocrystalline anisotropy was investigated in detail for the polycrystalline Ni50Mn25Ga25, Ni50Mn25Ga20Ti5 and Ni50Mn25Ga20Gd5 ferromagnetic shape memory alloys in the temperature range of 50–400 K. The effective anisotropy constant was estimated from a series of high field magnetization curves based on the fitting procedure according to the law of approach to magnetic saturation. The low temperature martensitic phase was found to have a significantly higher anisotropy energy in comparison to a high temperature austenitic phase, which was observed through a sudden, distinct drop of anisotropy energy. The calculated values of the effective anisotropy constant were comparable to the results published by other authors. Moreover, the strong influence of chemical composition on the first-order phase transition and the second-order ferromagnetic to the paramagnetic transition was revealed. Finally, the strong coupling between the temperature dependence of the coercive field and the temperature dependence of magnetocrystalline anisotropy was also shown and discussed in the present study.


2006 ◽  
Vol 438-440 ◽  
pp. 445-449 ◽  
Author(s):  
R.C. O’Handley ◽  
D.I. Paul ◽  
S.M. Allen ◽  
M. Richard ◽  
J. Feuchtwanger ◽  
...  

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