Magnetization, shape memory and hysteresis behavior of single and polycrystalline FeNiCoTi

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  • University of Illinois at Urbana-Champaign
  • Paderborn University
  • Tomsk State University
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Original languageEnglish
Pages (from-to)89-99
Number of pages11
JournalJournal of Magnetism and Magnetic Materials
Volume292
Publication statusPublished - Apr 2005
Externally publishedYes

Abstract

We report on the shape memory characteristics and magnetic behavior of polycrystalline and single crystalline FeNiCoTi. Predeforming the samples in the martensitic state and biasing of the martensite variants produced anisotropy in the magnetization behavior allowing the 'easy axis' to be identified as the 'a-axis' in the martensitic state. Based on these results, we provide an estimate of the magnetic anisotropy energy as 8.34×105 ergs/cm3. The results confirm the different magnetization behavior in the martensitic and austenitic states, and the shift in transformation temperatures upon application of a magnetic field. Shape memory strains near 2.5% are demonstrated under constant stress temperature cycling and upon heating at zero stress after deformation. We present a thermodynamics based theory that explains the origin of the hysteresis in this class of alloys emanating from the dissipation of energy due to plastic deformation. We predict the thermal hysteresis (135 K), and the shift in transformation temperature (14 K) with applied magnetic fields in agreement with the experimental results. The possibility of utilizing these classes of alloys as magnetic shape memory alloys is discussed.

Keywords

    Anisotropy, Energy dissipation, Magnetic shape memory

ASJC Scopus subject areas

Cite this

Magnetization, shape memory and hysteresis behavior of single and polycrystalline FeNiCoTi. / Sehitoglu, H.; Efstathiou, C.; Maier, H. J. et al.
In: Journal of Magnetism and Magnetic Materials, Vol. 292, 04.2005, p. 89-99.

Research output: Contribution to journalArticleResearchpeer review

Sehitoglu H, Efstathiou C, Maier HJ, Chumlyakov Y. Magnetization, shape memory and hysteresis behavior of single and polycrystalline FeNiCoTi. Journal of Magnetism and Magnetic Materials. 2005 Apr;292:89-99. doi: 10.1016/j.jmmm.2004.10.101
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title = "Magnetization, shape memory and hysteresis behavior of single and polycrystalline FeNiCoTi",
abstract = "We report on the shape memory characteristics and magnetic behavior of polycrystalline and single crystalline FeNiCoTi. Predeforming the samples in the martensitic state and biasing of the martensite variants produced anisotropy in the magnetization behavior allowing the 'easy axis' to be identified as the 'a-axis' in the martensitic state. Based on these results, we provide an estimate of the magnetic anisotropy energy as 8.34×105 ergs/cm3. The results confirm the different magnetization behavior in the martensitic and austenitic states, and the shift in transformation temperatures upon application of a magnetic field. Shape memory strains near 2.5% are demonstrated under constant stress temperature cycling and upon heating at zero stress after deformation. We present a thermodynamics based theory that explains the origin of the hysteresis in this class of alloys emanating from the dissipation of energy due to plastic deformation. We predict the thermal hysteresis (135 K), and the shift in transformation temperature (14 K) with applied magnetic fields in agreement with the experimental results. The possibility of utilizing these classes of alloys as magnetic shape memory alloys is discussed.",
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AU - Sehitoglu, H.

AU - Efstathiou, C.

AU - Maier, H. J.

AU - Chumlyakov, Y.

N1 - Funding Information: The work is partially supported by Air Force Office of Scientific Research, Directorate of Aerospace and Materials Sciences, Arlington, Virginia under Grant #F49620-01-1-0136, and also NSF Grants CMS-0332824 and CMS-0428428.

PY - 2005/4

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N2 - We report on the shape memory characteristics and magnetic behavior of polycrystalline and single crystalline FeNiCoTi. Predeforming the samples in the martensitic state and biasing of the martensite variants produced anisotropy in the magnetization behavior allowing the 'easy axis' to be identified as the 'a-axis' in the martensitic state. Based on these results, we provide an estimate of the magnetic anisotropy energy as 8.34×105 ergs/cm3. The results confirm the different magnetization behavior in the martensitic and austenitic states, and the shift in transformation temperatures upon application of a magnetic field. Shape memory strains near 2.5% are demonstrated under constant stress temperature cycling and upon heating at zero stress after deformation. We present a thermodynamics based theory that explains the origin of the hysteresis in this class of alloys emanating from the dissipation of energy due to plastic deformation. We predict the thermal hysteresis (135 K), and the shift in transformation temperature (14 K) with applied magnetic fields in agreement with the experimental results. The possibility of utilizing these classes of alloys as magnetic shape memory alloys is discussed.

AB - We report on the shape memory characteristics and magnetic behavior of polycrystalline and single crystalline FeNiCoTi. Predeforming the samples in the martensitic state and biasing of the martensite variants produced anisotropy in the magnetization behavior allowing the 'easy axis' to be identified as the 'a-axis' in the martensitic state. Based on these results, we provide an estimate of the magnetic anisotropy energy as 8.34×105 ergs/cm3. The results confirm the different magnetization behavior in the martensitic and austenitic states, and the shift in transformation temperatures upon application of a magnetic field. Shape memory strains near 2.5% are demonstrated under constant stress temperature cycling and upon heating at zero stress after deformation. We present a thermodynamics based theory that explains the origin of the hysteresis in this class of alloys emanating from the dissipation of energy due to plastic deformation. We predict the thermal hysteresis (135 K), and the shift in transformation temperature (14 K) with applied magnetic fields in agreement with the experimental results. The possibility of utilizing these classes of alloys as magnetic shape memory alloys is discussed.

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