High-temperature superelasticity in CoNiGa, CoNiAl, NiFeGa, and TiNi monocrystals

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Autoren

  • Yu I. Chumlyakov
  • I. V. Kireeva
  • E. Yu Panchenko
  • E. E. Timofeeva
  • Z. V. Pobedennaya
  • S. V. Chusov
  • I. Karaman
  • H. Maier
  • E. Cesari
  • V. A. Kirillov

Externe Organisationen

  • Tomsk State University
  • Texas A and M University
  • Universität Paderborn
  • University of the Balearic Islands
Forschungs-netzwerk anzeigen

Details

OriginalspracheEnglisch
Seiten (von - bis)1016-1036
Seitenumfang21
FachzeitschriftRussian physics journal
Jahrgang51
Ausgabenummer10
PublikationsstatusVeröffentlicht - Okt. 2008
Extern publiziertJa

Abstract

The influence of the crystal orientation on the thermoelastic martensitic transformations developing under load was investigated for Co 49Ni21Ga30, Co40Ni 33Al27, Co35Ni35Al30, Ni54Fe19Ga27, and Ti49.4Ni 50.6 (at. %) monocrystals. It has been shown that the superelastic temperature range depends on the crystal orientation and reaches a maximum for [001]-oriented crystals. In monophase crystals of Co49Ni 21Ga30, Co40Ni33Al27, Co35Ni35Al30, and Ni54Fe 19Ga27 (at. %), segregation of dispersion particles takes place at test temperatures T∈>∈623 K. A criterion for high-temperature superelasticity has been proposed which implies the attainment of high strength of the high-temperature phase due to a proper choice of the crystal orientation, deviation from stoichiometry, and segregation of dispersion particles.

ASJC Scopus Sachgebiete

Zitieren

High-temperature superelasticity in CoNiGa, CoNiAl, NiFeGa, and TiNi monocrystals. / Chumlyakov, Yu I.; Kireeva, I. V.; Panchenko, E. Yu et al.
in: Russian physics journal, Jahrgang 51, Nr. 10, 10.2008, S. 1016-1036.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Chumlyakov, YI, Kireeva, IV, Panchenko, EY, Timofeeva, EE, Pobedennaya, ZV, Chusov, SV, Karaman, I, Maier, H, Cesari, E & Kirillov, VA 2008, 'High-temperature superelasticity in CoNiGa, CoNiAl, NiFeGa, and TiNi monocrystals', Russian physics journal, Jg. 51, Nr. 10, S. 1016-1036. https://doi.org/10.1007/s11182-009-9143-5
Chumlyakov, Y. I., Kireeva, I. V., Panchenko, E. Y., Timofeeva, E. E., Pobedennaya, Z. V., Chusov, S. V., Karaman, I., Maier, H., Cesari, E., & Kirillov, V. A. (2008). High-temperature superelasticity in CoNiGa, CoNiAl, NiFeGa, and TiNi monocrystals. Russian physics journal, 51(10), 1016-1036. https://doi.org/10.1007/s11182-009-9143-5
Chumlyakov YI, Kireeva IV, Panchenko EY, Timofeeva EE, Pobedennaya ZV, Chusov SV et al. High-temperature superelasticity in CoNiGa, CoNiAl, NiFeGa, and TiNi monocrystals. Russian physics journal. 2008 Okt;51(10):1016-1036. doi: 10.1007/s11182-009-9143-5
Chumlyakov, Yu I. ; Kireeva, I. V. ; Panchenko, E. Yu et al. / High-temperature superelasticity in CoNiGa, CoNiAl, NiFeGa, and TiNi monocrystals. in: Russian physics journal. 2008 ; Jahrgang 51, Nr. 10. S. 1016-1036.
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title = "High-temperature superelasticity in CoNiGa, CoNiAl, NiFeGa, and TiNi monocrystals",
abstract = "The influence of the crystal orientation on the thermoelastic martensitic transformations developing under load was investigated for Co 49Ni21Ga30, Co40Ni 33Al27, Co35Ni35Al30, Ni54Fe19Ga27, and Ti49.4Ni 50.6 (at. %) monocrystals. It has been shown that the superelastic temperature range depends on the crystal orientation and reaches a maximum for [001]-oriented crystals. In monophase crystals of Co49Ni 21Ga30, Co40Ni33Al27, Co35Ni35Al30, and Ni54Fe 19Ga27 (at. %), segregation of dispersion particles takes place at test temperatures T∈>∈623 K. A criterion for high-temperature superelasticity has been proposed which implies the attainment of high strength of the high-temperature phase due to a proper choice of the crystal orientation, deviation from stoichiometry, and segregation of dispersion particles.",
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note = "Funding Information: The work has been supported in part the Russian Foundation for Basic Research, grants Nos. 05-08-17915-a and 08-08-91952 NNIO-a, by DFG-MA grant No. 1175/25-1, and by NSF grant No. 0805293.",
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TY - JOUR

T1 - High-temperature superelasticity in CoNiGa, CoNiAl, NiFeGa, and TiNi monocrystals

AU - Chumlyakov, Yu I.

AU - Kireeva, I. V.

AU - Panchenko, E. Yu

AU - Timofeeva, E. E.

AU - Pobedennaya, Z. V.

AU - Chusov, S. V.

AU - Karaman, I.

AU - Maier, H.

AU - Cesari, E.

AU - Kirillov, V. A.

N1 - Funding Information: The work has been supported in part the Russian Foundation for Basic Research, grants Nos. 05-08-17915-a and 08-08-91952 NNIO-a, by DFG-MA grant No. 1175/25-1, and by NSF grant No. 0805293.

PY - 2008/10

Y1 - 2008/10

N2 - The influence of the crystal orientation on the thermoelastic martensitic transformations developing under load was investigated for Co 49Ni21Ga30, Co40Ni 33Al27, Co35Ni35Al30, Ni54Fe19Ga27, and Ti49.4Ni 50.6 (at. %) monocrystals. It has been shown that the superelastic temperature range depends on the crystal orientation and reaches a maximum for [001]-oriented crystals. In monophase crystals of Co49Ni 21Ga30, Co40Ni33Al27, Co35Ni35Al30, and Ni54Fe 19Ga27 (at. %), segregation of dispersion particles takes place at test temperatures T∈>∈623 K. A criterion for high-temperature superelasticity has been proposed which implies the attainment of high strength of the high-temperature phase due to a proper choice of the crystal orientation, deviation from stoichiometry, and segregation of dispersion particles.

AB - The influence of the crystal orientation on the thermoelastic martensitic transformations developing under load was investigated for Co 49Ni21Ga30, Co40Ni 33Al27, Co35Ni35Al30, Ni54Fe19Ga27, and Ti49.4Ni 50.6 (at. %) monocrystals. It has been shown that the superelastic temperature range depends on the crystal orientation and reaches a maximum for [001]-oriented crystals. In monophase crystals of Co49Ni 21Ga30, Co40Ni33Al27, Co35Ni35Al30, and Ni54Fe 19Ga27 (at. %), segregation of dispersion particles takes place at test temperatures T∈>∈623 K. A criterion for high-temperature superelasticity has been proposed which implies the attainment of high strength of the high-temperature phase due to a proper choice of the crystal orientation, deviation from stoichiometry, and segregation of dispersion particles.

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