Shape Memory and Superelastic Technologies (SMST) (September 21-25, 2008): Temperature dependence of magnetic field-induced strain in Fe3Pt ferromagnetic SMA

5.4 Temperature dependence of magnetic field-induced strain in Fe3Pt ferromagnetic SMA

Monday, September 22, 2008: 3:15 PM
Room C (Palazzo dei Congressi di Stresa)
Prof. Tomoyuki Kakeshita , Department of Materials Science and Engineering, Graduate School of Engineering, Osaka University, Suita, Osaka, Japan
Takashi Fukuda , Department of Materials Science and Engineering, Graduate School of Engineering, Osaka University, Suita, Osaka, Japan
A partly ordered Fe3Pt exhibits a martensitic transformation from the L12-type cubic phase to a tetragonal martensite, which is frequently referred to as the FCT martensite. Below the transformation temperature of about 85K, the FCT martensite phase exhibits a large magnetic field-induced strain in association with rearrangement of martensite variants under the magnetic field. A part of the magnetic field-induced strain is reversible, being different behavior from the magnetic field-induced strain of Ni2MnGa. The magnitude of the reversible strain depends on temperature, and maximum value of about 1% is obtained at 20 K. Under a magnetic field, the variant whose easy axis lies in the field direction
 is the preferable variant, which grows consuming other variants. The fraction of the preferable variant at a temperature is higher in the specimen which is cooled down to the temperature under a magnetic field compared with the specimen
 which is cooled down to the same temperature under zero magnetic field followed by the application of the same magnetic field. Some fundamental physical properties, such as magnetocrstalline anisotropy and twinning stress, in Fe3Pt are also presented.