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Using eigenmoduli and eigenstates to evaluate the possibility of martensitic phase transformations
B. D. Anninab, N. I. Ostrosablina, R. I. Ugryumovab a Lavrentyev Institute of Hydrodynamics of Siberian Branch of the Russian Academy of Sciences, 630090, Novosibirsk, Russia
b Novosibirsk State University, 630090, Novosibirsk, Russia
Abstract:
The possibility of phase transitions (martensitic transformations) in shape-memory alloys is evaluated using the concept of eigenmoduli and eigenstates from the linear theory of elasticity. For alloys with cubic and hexagonal lattices, the matrices of elastic moduli and compl are given and expressions for their eigenmoduli and eigenstates are written. For cubic and hexagonal phases, the specific strain energy is presented as the sum of six independent terms corresponding to six orthogonal eigenstates. It is shown that depending on the ratio of eigenmoduli, there are six types of materials (alloys) with cubic and hexagonal symmetry. The specific strain energies in the cubic and hexagonal phases are compared. If the strain energy is greater in the hexagonal phase than in the cubic phase, the alloy can tend to return to its original state with lower energy. In addition, the strain energies in different phases can be compared using the formulas of the tensors closest in the Euclidean energy norm to cubic and hexagonal tensors. The energies are compared for some values of elastic constants.
Keywords:
eigenmoduli and eigenstates, shape-memory alloys, elastic moduli, compliances, cubic and hexagonal lattices, specific strain energy.
Received: 15.12.2020 Revised: 22.01.2021 Accepted: 25.01.2021
Citation:
B. D. Annin, N. I. Ostrosablin, R. I. Ugryumov, “Using eigenmoduli and eigenstates to evaluate the possibility of martensitic phase transformations”, Prikl. Mekh. Tekh. Fiz., 62:5 (2021), 5–14; J. Appl. Mech. Tech. Phys., 62:5 (2021), 707–716
Linking options:
https://www.mathnet.ru/eng/pmtf104 https://www.mathnet.ru/eng/pmtf/v62/i5/p5
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Abstract page: | 39 | References: | 10 | First page: | 4 |
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