Shape memory effect and high-temperature superelasticity in high-strength single crystals

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Autoren

  • Yu Chumlyakov
  • I. Kireeva
  • E. Panchenko
  • I. Karaman
  • H. J. Maier
  • E. Timofeeva

Externe Organisationen

  • Tomsk State University
  • Texas A and M University
  • Universität Paderborn
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Details

OriginalspracheEnglisch
Seiten (von - bis)S393-S398
FachzeitschriftJournal of alloys and compounds
Jahrgang577
AusgabenummerSUPPL. 1
PublikationsstatusVeröffentlicht - 23 Feb. 2012
Extern publiziertJa

Abstract

In the present study the temperature interval of superelasticity in Ti 49.4Ni50.6, Co49Ni21Ga30, Ni54Fe19Ga27 and Fe41Ni 28Co17Al11.5Ta2.5 (at%) single crystals are investigated. It is shown that it is necessary to produce materials with (i) a high yield stress level of the high-temperature phase of |σcrA| ∼ G/300-G/100 (G is shear modulus), and (ii) a low value of α = d|σcrM|/dT (|σcrM| is the critical stress required for stress-induced martensitic transformation) to achieve high-temperature superelasticity at T > 373 K. A high stress level of austenite |σcrA| can be obtained through selection of the crystal axis orientation, the stress state (tension vs. compression), variation of the chemical composition of the intermetallic compounds, and precipitation of dispersed particles. Low values of α are realized for crystal orientations providing maximum values for the transformation strain É0|.

ASJC Scopus Sachgebiete

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Shape memory effect and high-temperature superelasticity in high-strength single crystals. / Chumlyakov, Yu; Kireeva, I.; Panchenko, E. et al.
in: Journal of alloys and compounds, Jahrgang 577, Nr. SUPPL. 1, 23.02.2012, S. S393-S398.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Chumlyakov Y, Kireeva I, Panchenko E, Karaman I, Maier HJ, Timofeeva E. Shape memory effect and high-temperature superelasticity in high-strength single crystals. Journal of alloys and compounds. 2012 Feb 23;577(SUPPL. 1):S393-S398. doi: 10.1016/j.jallcom.2012.02.003
Chumlyakov, Yu ; Kireeva, I. ; Panchenko, E. et al. / Shape memory effect and high-temperature superelasticity in high-strength single crystals. in: Journal of alloys and compounds. 2012 ; Jahrgang 577, Nr. SUPPL. 1. S. S393-S398.
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abstract = "In the present study the temperature interval of superelasticity in Ti 49.4Ni50.6, Co49Ni21Ga30, Ni54Fe19Ga27 and Fe41Ni 28Co17Al11.5Ta2.5 (at%) single crystals are investigated. It is shown that it is necessary to produce materials with (i) a high yield stress level of the high-temperature phase of |σcrA| ∼ G/300-G/100 (G is shear modulus), and (ii) a low value of α = d|σcrM|/dT (|σcrM| is the critical stress required for stress-induced martensitic transformation) to achieve high-temperature superelasticity at T > 373 K. A high stress level of austenite |σcrA| can be obtained through selection of the crystal axis orientation, the stress state (tension vs. compression), variation of the chemical composition of the intermetallic compounds, and precipitation of dispersed particles. Low values of α are realized for crystal orientations providing maximum values for the transformation strain {\'E}0|.",
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AU - Chumlyakov, Yu

AU - Kireeva, I.

AU - Panchenko, E.

AU - Karaman, I.

AU - Maier, H. J.

AU - Timofeeva, E.

N1 - Funding information: This work was supported by the following research grants: RFBR , 09-03-00103-? , 10-03-00154-a , 10-08-92501 IK ; Federal Programs , 16.740.11.0462 , 14.740.11.0258 ; CRDF RUE1 - 2983-TO-10 .

PY - 2012/2/23

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N2 - In the present study the temperature interval of superelasticity in Ti 49.4Ni50.6, Co49Ni21Ga30, Ni54Fe19Ga27 and Fe41Ni 28Co17Al11.5Ta2.5 (at%) single crystals are investigated. It is shown that it is necessary to produce materials with (i) a high yield stress level of the high-temperature phase of |σcrA| ∼ G/300-G/100 (G is shear modulus), and (ii) a low value of α = d|σcrM|/dT (|σcrM| is the critical stress required for stress-induced martensitic transformation) to achieve high-temperature superelasticity at T > 373 K. A high stress level of austenite |σcrA| can be obtained through selection of the crystal axis orientation, the stress state (tension vs. compression), variation of the chemical composition of the intermetallic compounds, and precipitation of dispersed particles. Low values of α are realized for crystal orientations providing maximum values for the transformation strain É0|.

AB - In the present study the temperature interval of superelasticity in Ti 49.4Ni50.6, Co49Ni21Ga30, Ni54Fe19Ga27 and Fe41Ni 28Co17Al11.5Ta2.5 (at%) single crystals are investigated. It is shown that it is necessary to produce materials with (i) a high yield stress level of the high-temperature phase of |σcrA| ∼ G/300-G/100 (G is shear modulus), and (ii) a low value of α = d|σcrM|/dT (|σcrM| is the critical stress required for stress-induced martensitic transformation) to achieve high-temperature superelasticity at T > 373 K. A high stress level of austenite |σcrA| can be obtained through selection of the crystal axis orientation, the stress state (tension vs. compression), variation of the chemical composition of the intermetallic compounds, and precipitation of dispersed particles. Low values of α are realized for crystal orientations providing maximum values for the transformation strain É0|.

KW - Crystal growth

KW - High-temperature alloys

KW - Phase transitions

KW - Shape memory

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