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1. Modified Likhachev-Volkov  model  may be successfully used for the simulation of the strain variation during cooling and isothermal holding under stress.
2. To describe the strain variation on holding after active deformation, elastic energy stored during the transformation should be decreasd.

Simulation of recoverable strain variation during isothermal holding of the Ni51Ti49 alloy under various regimes

1. Modified Likhachev-Volkov model may be successfully used for the simulation of the strain variation during cooling and isothermal holding under stress. 2. To describe the strain variation on holding after active deformation, elastic energy stored during the transformation should be decreasd.
N.N. Resnina, A.M. Ivanov, F.S. Belyaev, A.E. Volkov, S.P. Belyaev
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Regardless of δ-ferrite fraction in the additively manufactured CrNi stainless, the increase in strain rate slows down the kinetics of strain-induced γ→α' martensitic transformation, but weakly influences the stress and strain, at which the macroscopic transformation stage starts.

Strain-rate dependent deformation behavior of additively manufactured stainless steel with different fractions of δ-ferrite

Regardless of δ-ferrite fraction in the additively manufactured CrNi stainless, the increase in strain rate slows down the kinetics of strain-induced γ→α' martensitic transformation, but weakly influences the stress and strain, at which the macroscopic transformation stage starts.
S.V. Astafurov, E.V. Melnikov, M.Y. Panchenko, K.A. Reunova, A.V. Luchin, E.A. Zagibalova, E.G. Astafurova, E.A. Kolubaev
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The increase in the specific electrical capacitance of C-matrices as a result of the introduction of the most efficient fillers is 250–450%, depending on the type of matrix, filler, and potential scan rate.

Carbon matrix nanostructured composites as a new type of supercapacitor electrode materials

The increase in the specific electrical capacitance of C-matrices as a result of the introduction of the most efficient fillers is 250–450%, depending on the type of matrix, filler, and potential scan rate.
Y.A. Zakharov, G.Y. Simenyuk, T.O. Sergina, N.V. Ivanova, T.A. Larichev, I.Y. Zykov, Y.N. Dudnikova
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The deposition of corrosion products on the surface of the alloy ZK60 creates the compressive internal stresses of types I and II.

Assessing residual stresses in the surface layer of the ZK60 alloy after an exposure to corrosion solution

The deposition of corrosion products on the surface of the alloy ZK60 creates the compressive internal stresses of types I and II.
E.D. Merson, V.A. Poluyanov, A.V. Polunin, P.N. Myagkikh, A.Y. Vinogradov, D.L. Merson
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Carbide/binder grain boundaries in a FIB lamella prepared from the WC-Co-Re cemented carbide were examined by high-angle annular dark field scanning transmission electron microscopy and energy dispersive X-ray spectroscopy at a high resolution. Rhenium was found to segregate at the grain boundaries forming complexions of 2 to 3 atomic monolayers, which presumably consist of mixed W-Re carbide.

Complexions at carbide / binder grain boundaries of Re-containing submicron cemented carbide

Carbide/binder grain boundaries in a FIB lamella prepared from the WC-Co-Re cemented carbide were examined by high-angle annular dark field scanning transmission electron microscopy and energy dispersive X-ray spectroscopy at a high resolution. Rhenium was found to segregate at the grain boundaries forming complexions of 2 to 3 atomic monolayers, which presumably consist of mixed W-Re carbide.
A.A. Zaitsev, A.A. Meledin
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We observed the ordered phase particle experimentally by the TEM method. The temperature of the order–disorder phase transition in the Cu-5.9Pd alloy was estimated as Tc ≈ 340°С.

Signs of the presence of an ordered phase in the Cu-5.9 at.% Pd alloy after its long-term annealing at a moderate temperature

We observed the ordered phase particle experimentally by the TEM method. The temperature of the order–disorder phase transition in the Cu-5.9Pd alloy was estimated as Tc ≈ 340°С.
О.С. Новикова, А.Е. Костина, Е.Г. Волкова, Ю.А. Саламатов, А.В. Глухов, А.Ю. Волков, В.В. Марченков, В.С. Гавико, Ю.М. Устюгов
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