Shape memory effect and high-temperature superelasticity in high-strength single crystals Y. I. Chumlyakov, I. V. Kireeva, E. Y. Panchenko [et.al.]
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ArticleSubject(s): эффект памяти формы | монокристаллы | жаропрочные сплавы | высокотемпературная сверхэластичность | фазовые переходыGenre/Form: статьи в журналах Online resources: Click here to access online
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Journal of alloys and compounds Vol. 577. P. 393-398Abstract: 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 σcr A G/300-G/100 (G is shear modulus), and (ii) a low value of α = dσcr M/dT (σcr M 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 σcr A 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.
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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 σcr A G/300-G/100 (G is shear modulus), and (ii) a low value of α = dσcr M/dT (σcr M 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 σcr A 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.
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