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Structural and mechanical properties of NiTiAg shape memory alloys: ab-initio study
The austenite phase of Ni 50− x Ti 50 Ag x for different concentrations ( x = 1, 1.5, 2, 3, 5, 7, 8, 10) has been analyzed in this work. The ground state, structural, and mechanical characteristics of Ni 50− x Ti 50 Ag x for various concentrations are examined under ambient conditions. From total en...
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Published in: | Modelling and simulation in materials science and engineering 2023-09, Vol.31 (6), p.65004 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The austenite phase of Ni
50−
x
Ti
50
Ag
x
for different concentrations (
x
= 1, 1.5, 2, 3, 5, 7, 8, 10) has been analyzed in this work. The ground state, structural, and mechanical characteristics of Ni
50−
x
Ti
50
Ag
x
for various concentrations are examined under ambient conditions. From total energy as well as formation energy calculations, it is found that the stability of Ni
50−
x
Ti
50
Ag
x
austenite phase is increased up to
x
= 5 and after that it becomes unstable in nature. These results are in good agreement with our experimental results. The experimental and other theoretical results agree with the estimated lattice parameter values. The x-ray diffraction and differential scanning calorimetry reveal the phases formed and transformation characteristics of NiTiAg alloys. The elastic constants, bulk modulus, shear modulus, Poisson’s ratio, and elastic anisotropy factor of Ni
50−
x
Ti
50
Ag
x
are examined at ambient conditions for different concentrations. From elastic constant calculations, it is also found that the austenite phase of Ni
50−
x
Ti
50
Ag
x
is mechanically stable up to
x
= 5 and after that it does not obey Born–Huang criteria and becomes unstable. The Ni
45
Ti
50
Ag
5
composition is found to be the stiffest and hardest material. According to Poisson’s ratio calculations, Ni
50−
x
Ti
50
Ag
x
shows that the Ti–Ag, Ni–Ag bonding is more directed in nature. The austenite phase of Ni
50−
x
Ti
50
Ag
x
is more incompressible because the Poisson’s ratio is nearly equal to the optimum value (0.5). |
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ISSN: | 0965-0393 1361-651X |
DOI: | 10.1088/1361-651X/acde94 |