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Molecular dynamics simulation is an effective computer simulation method. However, owing to the lack of suitable interatomic potential of multicomponent alloys, the application of molecular dynamics simulation is limited. The development of interatomic potential of multicomponent alloys has always been challenging. In this work, under the framework of EAM model, a construction method of interatomic potential suitable for ternary ordered alloys is proposed, and a new interatomic potential of Ti2AlNb alloys suitable for atomic-scale mechanical behavior simulation is developed. The potential can well reproduce the elastic constants of B2-Ti2AlNb, unrelaxation vacancy formation energy, substitutional atom formation energy, transposition atom formation energy, surface energy and cohesive energy of three ordered phase (B2, D019 and O phases ) in different volumes. To further test the potential functions, 1) the E-V curve of B2 phase is calculated, and the result is well consistent with Rose curve; 2) the melting transformation process of B2 phase is studied by molecular dynamics simulation, and the results roughly reflect the experimental fact. The present work provides a way to develop the interatomic potential of multicomponent alloys, and a option for the workers who simulate and calculate the Ti2AlNb alloys as well.
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Keywords:
- embedded atom method potential /
- Ti2AlNb alloys /
- defects
[1] Deringer V, Csanyi G 2017 Phys. Rev. B 95 094203
Google Scholar
[2] Alizadeh Z, Mohammadizadeh M R 2019 Physica C 558 7
Google Scholar
[3] Jordan M I, Mitchell T M 2015 Science 349 255
Google Scholar
[4] Smith J S, Nebgen B, Mathew N, Chen J, Lubbers N, Burakovsky L, Tretiak S, Nam H A, Germann T, Fensin S, Barros K 2021 Nat. Commun. 12 1257
Google Scholar
[5] Artrith N, Urban A 2016 Comput. Mater. Sci. 114 135
Google Scholar
[6] Kumpfert J 2001 Adv. Eng. Mater. 3 851
Google Scholar
[7] Boehlert C J, Majumdar B S 1999 Metall. Mater. Trans. A 30 2305
Google Scholar
[8] 冯艾寒, 李渤渤, 沈军 2011 材料与冶金学报 10 30
Google Scholar
Feng A H, Li B B, Shen J 2011 J. Mater. Metall. 10 30
Google Scholar
[9] Gogia T K, Nandy T K, Banerjee D, Carisey T, Strudel J L, Franchet J M 1998 Intermetallics 6 741
Google Scholar
[10] Banerjee D, Gogia A K, Nandi T K, Joshi V A 1988 Acta Metall. 36 871
Google Scholar
[11] Pathak A, Singh A K 2015 Solid State Commun. 204 9
Google Scholar
[12] Daw M S, Baskes M I 1984 Phys. Rev. B 29 6443
Google Scholar
[13] Cheng C, Ma Y L, Bao Q L, Wang X, Sun J X, Zhou G, Wang H, Liu Y X, Xu D S 2019 Comput. Mater. Sci. 173 109432
Google Scholar
[14] Johnson R A 1989 Phys. Rev. B 39 12554
Google Scholar
[15] Voter A F 1994 Intermetallic Compounds (New York: Wiley) pp77—80
[16] Mishin Y, Mehl M J 2002 Phys. Rev. B 65 224114
Google Scholar
[17] Ravi C, Vajeeston P, Mathijaya S, Asokamani R 1999 Phys. Rev. B:Condens. Matter. 60 683
Google Scholar
[18] Kittel C 1976 Introduction to Solid State Physics (New Jersey: John Wiley & Sons) pp57–58
[19] Weast R C 1984 Handbook of Chemistry and Physics (Boca Raton: Chemical Rubber) p64
[20] Johnson R A 1972 Phys. Rev. B 6 2094
Google Scholar
[21] Oh D J, Johnson R A 2011 Mater. Res. 3 471
Google Scholar
[22] Bolef D I 1961 Appl. Phys. 32 100
Google Scholar
[23] Agrawal A, Mishra R, Ward L, Flores K M, Windl W 2013 Modell. Simul. Mater. Sci. Eng. 21 085001
Google Scholar
[24] Farkas D 1999 Modell. Simul Mater. Sci. Eng. 4 23
Google Scholar
[25] Rose J H, Smith J R, Guinea F, Ferrante J 1984 Phys. Rev. B 29 2963
Google Scholar
[26] Julius C S, Martin P 2006 J. Phase Equilib. Diffus. 27 255
Google Scholar
[27] Vasudevan V K, Yang J, Woodfield A P 1996 Scr. Mater. 35 1033
Google Scholar
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图 1 Ti2AlNb的EAM势 (a) 电子密度分布函数; (b) 嵌入能函数; (c) 同种原子间的对势; (d) 异种原子间的对势
Figure 1. EAM potential for Ti2AlNb: (a) Electron density function; (b) embedding energy function; (c) pair potentials between same types of atoms; (d) pair potentials between different types of atoms.
图 2 B2-Ti2AlNb单空位形成能与双空位形成能
Figure 2. Mono-vacancy formation energies and di-vacancy formation energies for B2-Ti2AlNb.
图 3 B2-Ti2AlNb原子位置换位示意图
Figure 3. Atom position transposition diagram for B2-Ti2AlNb.
图 4 B2-Ti2AlNb置换原子形成能的误差
Figure 4. Deviations of substitutional atom formation energies for B2-Ti2AlNb.
图 5 B2-Ti2AlNb换位原子形成能的误差
Figure 5. Deviations of transposition atom formation energies for B2-Ti2AlNb.
图 6 B2-Ti2AlNb的E-V曲线与Rose曲线
Figure 6. E-V curve and Rose curve for B2-Ti2AlNb.
图 7 Ti2AlNb合金的E-V曲线 (a) B2相; (b) D019相; (c) O相
Figure 7. E-V curve of Ti2AlNb alloys: (a) B2 phase; (b) D019 phase; (c) O phase.
图 8 B2相的每个原子的体积随温度的变化
Figure 8. Volume variation of each atom for B2 phase as functions of temperature.
图 9 B2相随温度变化的截面快照 (a) 296 K; (b) 754 K; (c) 1428 K; (d) 1390 K; (e) 1449 K; (f) 1728 K
Figure 9. Cross-section snapshots for
B2 phase as functions of temperature: (a) 296 K; (b) 754 K; (c) 1428 K; (d) 1390 K; (e) 1449 K; (f) 1728 K. 表 1 B2-Ti2AlNb的晶格常数和生成焓(单位: eV)
Table 1. Lattice constants and formation enthalpy for B2-Ti2AlNb (in eV).
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表 3 Ti2AlNb合金EAM势的拟合参数
Table 3. Fitting parameters of EAM potential for Ti2AlNb alloys.
$ \phi \left({r}_{\mathrm{T}\mathrm{i}\mathrm{A}\mathrm{l}}\right) $ $ \phi \left({r}_{\mathrm{T}\mathrm{i}\mathrm{N}\mathrm{b}}\right) $ $ \phi \left({r}_{\mathrm{N}\mathrm{b}\mathrm{A}\mathrm{l}}\right) $ Parameter value Parameter value Parameter value $ \alpha $ –2.1129 $ \alpha $ –4.2151 $ \alpha $ –0.2797 $ \beta $ –1.3742 $ \beta $ –6.6808 $ \beta $ –2.5122 $ \gamma $ 0.2705 $ \gamma $ 1.4339 $ \gamma $ 1.6140 $ \epsilon $ 0.1758 $ \epsilon $ –0.0008 $ \epsilon $ 0.1140 $ \sigma $ –2.3191 $ \sigma $ –1.4062 $ \sigma $ –1.6132 $ \mu $ 0.0516 $ \mu $ 0.2694 $ \mu $ 0.4012
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表 4 B2-Ti2AlNb的弹性常数(单位: GPa)
Table 4. Elastic constants for B2-Ti2AlNb (in GPa).
C11 C33 C44 C66 C12 C13 ABINIT[11] 136 — 81 — 100 — DFT 153.20 147.83 69.36 71.86 133.42 97.62 This work 195.82 178.95 64.35 66.83 136.92 127.04
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表 5 B2-Ti2AlNb单空位形成能和双空位形成能(单位: eV)
Table 5. Mono-vacancy formation energies and di-vacancy formation energies for B2-Ti2AlNb (in eV).
DFT This work This-lmp EAM-fa $ {E}_{\mathrm{v}}^{\mathrm{f}} $ Ti 2.879 2.283 2.283 1.343 Al 2.859 3.265 3.265 1.391 Nb 2.194 1.763 1.657 4.919 $ {E}_{\mathrm{d}}^{\mathrm{f}} $ TiTi-1 5.454 4.503 4.498 2.562 TiTi-2 5.854 4.539 4.533 2.777 TiTi-3 5.688 4.570 4.567 2.724 TiAl-1 5.623 5.434 5.434 4.014 TiNb-1 4.731 3.980 3.980 3.699 AlNb-1 4.710 4.854 4.854 4.777
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表 6 B2-Ti2AlNb置换原子和换位原子形成能(单位: eV)
Table 6. Substitutional atom and transposition atom formation energies for B2-Ti2AlNb (in eV).
DFT This work This-lmp EAM-fa $ {E}_{\mathrm{o}}^{\mathrm{f}} $ $ {\mathrm{T}\mathrm{i}}_{\mathrm{A}\mathrm{l}} $ 1.046 0.976 0.976 –2.863 $ {\mathrm{T}\mathrm{i}}_{\mathrm{N}\mathrm{b}} $ –0.384 –0.418 –0.418 –2.440 $ {\mathrm{A}\mathrm{l}}_{\mathrm{T}\mathrm{i}} $ 0.268 0.433 0.433 –1.164 $ {\mathrm{A}\mathrm{l}}_{\mathrm{N}\mathrm{b}} $ –1.310 –1.216 –1.216 –1.113 $ {\mathrm{N}\mathrm{b}}_{\mathrm{T}\mathrm{i}} $ 0.638 0.624 0.624 –7.439 $ {\mathrm{N}\mathrm{b}}_{\mathrm{A}\mathrm{l}} $ 1.522 1.289 1.289 0.911 $ {E}_{\mathrm{e}}^{\mathrm{f}} $ TiAl 1.097 1.181 1.181 –4.142 TiNb 0.270 0.191 0.191 –9.213 AlNb 0.123 0.172 0.172 –0.571 Clo 1.078 1.132 1.132 –3.169 Ant 0.453 0.413 0.413 –10.752
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表 7 B2-Ti2AlNb的表面能(单位: eV)
Table 7. Surface energies for
B2-Ti2AlNb (in eV). DFT This work This-lmp EAM-fa $ {E}_{\mathrm{s}\mathrm{u}\mathrm{r}}^{\mathrm{f}} $ (100) 2.056 2.298 2.273 1.705 (110) 1.937 2.194 2.170 1.620 (100)′ 1.844 — 1.923 0.484 (110)′ 1.661 — 1.750 –11.000
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表 8 Ti2AlNb合金的内聚能(单位: eV)
Table 8. Cohesive energies for Ti2AlNb alloys (in eV).
VB2 60% 67% 75% 83% 91% 1 110% 120% 130% 142% 154% E-DFT –3.22 –4.13 –4.75 –5.14 –5.35 –5.42 –5.37 –5.22 –5.02 –4.77 –4.48 $ V_{{\rm D0}_{19}} $ 57% 64% 72% 81% 90% 1 111% 122% 134% 147% 160% E-DFT –2.55 –3.78 –4.60 –5.10 –5.37 –5.44 –5.38 –5.21 –4.96 –4.66 –4.32 VO 58% 65% 73% 81% 90% 1 110% 121% 133% 145% 158% E-DFT –2.79 –3.92 –4.69 –5.16 –5.41 –5.48 –5.42 –5.26 –5.03 –4.74 –4.42
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[1] Deringer V, Csanyi G 2017 Phys. Rev. B 95 094203
Google Scholar
[2] Alizadeh Z, Mohammadizadeh M R 2019 Physica C 558 7
Google Scholar
[3] Jordan M I, Mitchell T M 2015 Science 349 255
Google Scholar
[4] Smith J S, Nebgen B, Mathew N, Chen J, Lubbers N, Burakovsky L, Tretiak S, Nam H A, Germann T, Fensin S, Barros K 2021 Nat. Commun. 12 1257
Google Scholar
[5] Artrith N, Urban A 2016 Comput. Mater. Sci. 114 135
Google Scholar
[6] Kumpfert J 2001 Adv. Eng. Mater. 3 851
Google Scholar
[7] Boehlert C J, Majumdar B S 1999 Metall. Mater. Trans. A 30 2305
Google Scholar
[8] 冯艾寒, 李渤渤, 沈军 2011 材料与冶金学报 10 30
Google Scholar
Feng A H, Li B B, Shen J 2011 J. Mater. Metall. 10 30
Google Scholar
[9] Gogia T K, Nandy T K, Banerjee D, Carisey T, Strudel J L, Franchet J M 1998 Intermetallics 6 741
Google Scholar
[10] Banerjee D, Gogia A K, Nandi T K, Joshi V A 1988 Acta Metall. 36 871
Google Scholar
[11] Pathak A, Singh A K 2015 Solid State Commun. 204 9
Google Scholar
[12] Daw M S, Baskes M I 1984 Phys. Rev. B 29 6443
Google Scholar
[13] Cheng C, Ma Y L, Bao Q L, Wang X, Sun J X, Zhou G, Wang H, Liu Y X, Xu D S 2019 Comput. Mater. Sci. 173 109432
Google Scholar
[14] Johnson R A 1989 Phys. Rev. B 39 12554
Google Scholar
[15] Voter A F 1994 Intermetallic Compounds (New York: Wiley) pp77—80
[16] Mishin Y, Mehl M J 2002 Phys. Rev. B 65 224114
Google Scholar
[17] Ravi C, Vajeeston P, Mathijaya S, Asokamani R 1999 Phys. Rev. B:Condens. Matter. 60 683
Google Scholar
[18] Kittel C 1976 Introduction to Solid State Physics (New Jersey: John Wiley & Sons) pp57–58
[19] Weast R C 1984 Handbook of Chemistry and Physics (Boca Raton: Chemical Rubber) p64
[20] Johnson R A 1972 Phys. Rev. B 6 2094
Google Scholar
[21] Oh D J, Johnson R A 2011 Mater. Res. 3 471
Google Scholar
[22] Bolef D I 1961 Appl. Phys. 32 100
Google Scholar
[23] Agrawal A, Mishra R, Ward L, Flores K M, Windl W 2013 Modell. Simul. Mater. Sci. Eng. 21 085001
Google Scholar
[24] Farkas D 1999 Modell. Simul Mater. Sci. Eng. 4 23
Google Scholar
[25] Rose J H, Smith J R, Guinea F, Ferrante J 1984 Phys. Rev. B 29 2963
Google Scholar
[26] Julius C S, Martin P 2006 J. Phase Equilib. Diffus. 27 255
Google Scholar
[27] Vasudevan V K, Yang J, Woodfield A P 1996 Scr. Mater. 35 1033
Google Scholar
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