“…12 If the martensitic transformation is tuned to be coupled with the magnetic transition, i.e., the magnetostructural transformation, the MCE becomes giant. 3,12 Currently, large MCE has been observed in single crystals, 3 polycrystalline bulk alloys, [12][13][14][15][16][17][18][19][20] and melt-spun ribbons 21,22 with magneto-unistructural transformation. The highest DS M of À86 J kg À1 K À1 was achieved in singlecrystalline Ni 55 Mn 20 Ga 25 alloy at a magnetic field change of about 5 T. 3 However, the high cost and complexity associated with the fabrication of single crystals becomes an unavoidable hindrance for practical applications.…”
“…12 If the martensitic transformation is tuned to be coupled with the magnetic transition, i.e., the magnetostructural transformation, the MCE becomes giant. 3,12 Currently, large MCE has been observed in single crystals, 3 polycrystalline bulk alloys, [12][13][14][15][16][17][18][19][20] and melt-spun ribbons 21,22 with magneto-unistructural transformation. The highest DS M of À86 J kg À1 K À1 was achieved in singlecrystalline Ni 55 Mn 20 Ga 25 alloy at a magnetic field change of about 5 T. 3 However, the high cost and complexity associated with the fabrication of single crystals becomes an unavoidable hindrance for practical applications.…”
“…The preparation and subsequent heat treatment of the polycrystalline ingots are the same as those in Refs. [15] and [16]. The x-ray powder diffraction measurements were investigated with Cu Kα radiation to prove the present samples crystallised in the non-modulated tetragonal martensitic structure at room temperature without secondary phase.…”
Section: Methodsmentioning
confidence: 92%
“…The x-ray powder diffraction measurements were investigated with Cu Kα radiation to prove the present samples crystallised in the non-modulated tetragonal martensitic structure at room temperature without secondary phase. [15,16] Magnetisation data were measured in fields from 0 to 2 T by vibrating sample magnetometer (VSM). The measurements of heating and cooling isothermal magnetisation curves were carried out by the following steps: at first, the sample was cooled to temperatures far below the Curie temperature T C and then heated to temperature near T C , after that the measurement of the isothermal magnetisation (M -H) curve began.…”
Section: Methodsmentioning
confidence: 99%
“…However, magnetic refrigeration cycle includes both heating and cooling processes and our previous studies have indicated that the magnetic entropy change could be different during heating and cooling. [15] Therefore comprehensive evaluation of hysteresis loss in Ni-Mn-Ga alloys cannot be given by research of heating or cooling process independently. Unfortunately, reports on the magnetic hysteresis of Heusler alloys usually focused on only one process, heating and cooling isothermal magnetisation processes are rarely studied together.…”
Fu Bin(傅 斌) a) , Long Yi(龙 毅) a) , Duan Jing-Fang(段静芳) a) , Wang Chao-Lun(王超伦) a) , Chang Yong-Qin(常永勤) a) , Ye Rong-Chang(叶荣昌) a) , and Wu Guang-Heng(吴光恒) b)
“…The aforementioned record-breaking values of magnetostrain, the high values of estimated magnetocaloric effect [56][57][58], and the effect of twinning-strain-induced rotation of the magnetization vector [59][60][61] are the phenomena in the focus of current research and development.…”
Abstract. The giant magnetically-induced deformation of ferromagnetic shape memory alloys results from the magnetic field-induced rearrangement of twinned martensite under the magnetic field. This deformation is conventionally referred to as the magnetic-field-induced-strain (MFIS). The MFIS is comparable in value with the spontaneous deformation of crystal lattice during the martensitic transformation of an alloy. Although the first observations of MFIS were reported more than 30 years ago, it has got a world-wide interest 20 years later after the creation of the Ni-Mn-Ga alloy system with its practically important room-temperature martensitic structure and experimental evidence of the large magnetostriction. The underlying physics as well as necessary and sufficient conditions for the observation of MFIS are the main focus of this chapter. A magnetostrictive mechanism of the unusual magnetic and magnetomechanical effects observed in Ni-Mn-Ga alloys is substantiated and a framework of consistent theory of these effects is outlined starting from the fundamental conception of magnetoelasticity and the commonly known principles of ferromagnetism and linear elasticity theories. A reasonable agreement between the theoretical deductions and available experimental data is demonstrated and, in this way, a key role of magnetoelastic coupling in the magnetomechanical behavior of Ni-Mn-Ga alloys is proved. A correspondence of magnetostrictive mechanism to the crystallographic features of MFIS and the basic relationships of the thermodynamics of solids are discussed.
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