基于原子模拟的金属Fe晶界能与晶界取向相关性分析
收稿日期: 2023-04-17
修回日期: 2023-09-06
网络出版日期: 2023-09-28
基金资助
国家自然科学基金项目(52065045);江西省杰出青年人才计划项目(20192BCBL23002)
Analysis of the Correlation Between the Energy and Crystallographic Orientation of Grain Boundaries in Fe Based on Atomistic Simulations
Received date: 2023-04-17
Revised date: 2023-09-06
Online published: 2023-09-28
Supported by
National Natural Science Foundation of China(52065045);Program Foundation for Distinguished Young Scholars of Jiangxi(20192BCBL23002)
晶界能(γ)会显著影响金属材料的诸多物理和力学性能,然而bcc金属内γ与晶界取向间相关性特征的认识仍非常有限。为揭示这些潜在特征,本研究采用截断球状双晶分子动力学模型,计算了bcc金属Fe内涵盖0°~180°取向差角(θ)、40个取向差轴( O )共1568组倾斜晶界的能量,统计性分析了γ与晶界取向参数的相关性并揭示了相关机理。结果表明,对于具有不同 O 的晶界,γ随θ的变化趋势在大角度范围内会存在显著差异;从统计性角度来看,γ在θ和偏转角较小时整体上随这2类角度的增大而提高,随后整体保持平稳。非重位点阵晶界的能量并不高于重位点阵(coincidence site lattice,CSL)晶界,在较小θ范围内随θ的变化趋势与CSL晶界相同。当 O 从取向投影三角形的内部向边部再向顶点变化时,倾斜晶界结构的对称性整体上逐渐升高从而对应能量逐渐降低,<111>顶点附近的能量整体最低。具有低Miller指数或高密排晶界面的晶界并不一定具有较低能量,γ整体上随晶界面对应表面能的增大而升高直至整体保持平稳。γ与重位因子(Σ)整体上无可见相关性,但固定 O 下γ(θ)曲线上的能量低谷一般都位于具有极小Σ的晶界。此外,还发现bcc金属中γ与晶界取向之间潜在的相关性及规律与fcc金属部分相似或相同。
黄曾鑫 , 蒋逸航 , 赖春明 , 吴庆捷 , 刘大海 , 杨亮 . 基于原子模拟的金属Fe晶界能与晶界取向相关性分析[J]. 金属学报, 2024 , 60(9) : 1289 -1298 . DOI: 10.11900/0412.1961.2023.00172
The grain boundary (GB) energy is one of the fundamental structure-dependent properties of GB and plays a crucial role in the GB-related behaviors and properties of polycrystalline materials. An in-depth understanding of GB energy will help to explore the corresponding mechanisms and provide significant guidance for tailoring material properties based on GB engineering. The crystallographic orientation of GB strongly dominates the GB energy. However, a relatively comprehensive understanding of the orientation dependence of the GB energy is still lacking, especially for bcc materials. In this study, the energies of 1568 tilt GBs in bcc Fe, which covers the misorientation angle (θ) of 0°-180° and 40 distinct misorientation axes ( O ), were computed using the cutoff sphere bicrystal molecular dynamics model. The energy dataset was used to statistically analyze the correlation between GB energy (γ) and GB crystallographic orientation, thereby revealing the underlying mechanisms. The results show that the tendencies of γ-θ correlationcan be considerably different in the high-angle range for GBs with distinct O. Statistically, GB energies increase with θ and disorientation angle in the low-angle range and then level off for higher angles. The energies for noncoincident site lattice (non-CSL) GBs are not necessarily higher than those of CSL GBs and follow the same trend in the low-θ range as CSL GBs. The energies of the tilt GBs decrease with the variation of O from the central regions to the edge and then the corners of the stereographic triangle due to the increasing tendency of the symmetry of the boundary structure. Therefore, the lowest energies are observed for GBs with O close to <111>. Relatively low energies are not observed for GBs terminated by low-index or dense planes. The GB energy shows an overall increasing trend with the surface energy of the boundary plane until a plateau in the GB energy is reached. No distinct correlation is observed between the GB energy and coincidence index (Σ) value. However, the cusp in the γ(θ) curve for GBs with a common O is found to be generally located at the GB with a much lower Σ than its neighboring GBs. Additionally, the potential correlations and laws concerning GB energy and its crystallographic orientation for bcc metals are observed to be partially similar or consistent with those of fcc metals.
| 1 | Read W T, Shockley W. Dislocation models of crystal grain boundaries [J]. Phys. Rev., 1950, 78: 275 |
| 2 | Liu F, Kirchheim R. Nano-scale grain growth inhibited by reducing grain boundary energy through solute segregation [J]. J. Cryst. Growth, 2004, 264: 385 |
| 3 | Hu J, Shi Y N, Sauvage X, et al. Grain boundary stability governs hardening and softening in extremely fine nanograined metals [J]. Science, 2017, 355: 1292 |
| 4 | Humphreys J, Rohrer G S, Rollett A D. Recrystallization and Related Annealing Phenomena [M]. 3rd Ed., Amsterdam: Elsevier, 2017: 294 |
| 5 | Xu K, Liang T, Zhang Z S, et al. Grain boundary and misorientation angle-dependent thermal transport in single-layer MoS2 [J]. Nanoscale, 2022, 14: 1241 |
| 6 | Rohrer G S. Grain boundary energy anisotropy: A review [J]. J. Mater. Sci., 2011, 46: 5881 |
| 7 | Coffman V R, Sethna J P. Grain boundary energies and cohesive strength as a function of geometry [J]. Phys. Rev., 2008, 77B: 44111 |
| 8 | Olmsted D L, Foiles S M, Holm E A. Survey of computed grain boundary properties in face-centered cubic metals: I. Grain boundary energy [J]. Acta Mater., 2009, 57: 3694 |
| 9 | Sutton A P, Banks E P, Warwick A R. The five-dimensional parameter space of grain boundaries [J]. Proc. Roy. Soc., 2015, 471A: 20150442 |
| 10 | Gjostein N A, Rhines F N. Absolute interfacial energies of [001] tilt and twist grain boundaries in copper [J]. Acta Metall., 1959, 7: 319 |
| 11 | Feng Y X, Shang J X, Liu Z H, et al. The energy and structure of (110) twist grain boundary in tungsten [J]. Appl. Surf. Sci., 2015, 357: 262 |
| 12 | Yang C C, Rollett A D, Mullins W W. Measuring relative grain boundary energies and mobilities in an aluminum foil from triple junction geometry [J]. Scr. Mater., 2001, 44: 2735 |
| 13 | Wolf D. Structure-energy correlation for grain boundaries in F.C.C. metals—I. Boundaries on the (111) and (100) planes [J]. Acta Metall., 1989, 37: 1983 |
| 14 | Wolf D. Structure-energy correlation for grain boundaries in F.C.C. metals—II. Boundaries on the (110) and (113) planes [J]. Acta Metall., 1989, 37: 2823 |
| 15 | Wolf D. Structure-energy correlation for grain boundaries in F.C.C. metals—III. Symmetrical tilt boundaries [J]. Acta Metall. Mater., 1990, 38: 781 |
| 16 | Liang C P, Wang W Q, Tang S, et al. Molecular dynamics simulation of symmetrical tilt grain boundary of body-centered cubic tungsten [J]. Chin. J. Nonferrous Met., 2021, 31: 1757 |
| 梁超平, 王文琦, 唐 赛 等. 钨对称倾斜晶界的分子动力学计算模拟 [J]. 中国有色金属学报, 2021, 31: 1757 | |
| 17 | Tschopp M A, McDowell D L. Asymmetric tilt grain boundary structure and energy in copper and aluminium [J]. Philos. Mag., 2007, 87: 3871 |
| 18 | Wolf D. On the relationship between symmetrical tilt, twist, “special”, and “favored” grain boundaries [J]. J. Phys. Coll., 1985, 46: C4-197 |
| 19 | Merkle K L. High-resolution electron microscopy of grain boundaries [J]. Interface Sci., 1995, 2: 311 |
| 20 | Yang L, Lai C M, Li S Y. Atomistic simulations of energies for arbitrary grain boundaries. Part II: Statistical analysis of energies for tilt and twist grain boundaries [J]. Comput. Mater. Sci., 2019, 162: 268 |
| 21 | Kim H K, Ko W S, Lee H J, et al. An identification scheme of grain boundaries and construction of a grain boundary energy database [J]. Scr. Mater., 2011, 64: 1152 |
| 22 | Ratanaphan S, Olmsted D L, Bulatov V V, et al. Grain boundary energies in body-centered cubic metals [J]. Acta Mater., 2015, 88: 346 |
| 23 | Ratanaphan S, Boonkird T, Sarochawikasit R, et al. Atomistic simulations of grain boundary energies in tungsten [J]. Mater. Lett., 2017, 186: 116 |
| 24 | Lee B J, Choi S H. Computation of grain boundary energies [J]. Model. Simul. Mater. Sci. Eng., 2004, 12: 621 |
| 25 | Li S Y, Yang L, Lai C M. Atomistic simulations of energies for arbitrary grain boundaries. Part I: Model and validation [J]. Comput. Mater. Sci., 2019, 161: 330 |
| 26 | Morawiec A. Method to calculate the grain boundary energy distribution over the space of macroscopic boundary parameters from the geometry of triple junctions [J]. Acta Mater., 2000, 48: 3525 |
| 27 | Li J, Dillon S J, Rohrer G S. Relative grain boundary area and energy distributions in nickel [J]. Acta Mater., 2009, 57: 4304 |
| 28 | Lee B J, Baskes M I, Kim H, et al. Second nearest-neighbor modified embedded atom method potentials for bcc transition metals [J]. Phys. Rev., 2001, 64B: 184102 |
| 29 | Plimpton S. Fast parallel algorithms for short-range molecular dynamics [J]. J. Comput. Phys., 1995, 117: 1 |
| 30 | Sutton A P, Balluffi R W. On geometric criteria for low interfacial energy [J]. Acta Metall., 1987, 35: 2177 |
| 31 | Yu Q, Nosonovsky M, Esche S K. Monte Carlo simulation of grain growth of single-phase systems with anisotropic boundary energies [J]. Int. J. Mech. Sci., 2009, 51: 434 |
| 32 | Chun Y B, Semiatin S L, Hwang S K. Monte Carlo modeling of microstructure evolution during the static recrystallization of cold-rolled, commercial-purity titanium [J]. Acta Mater., 2006, 54: 3673 |
| 33 | Wolf D. Structure and energy of general grain boundaries in bcc metals [J]. J. Appl. Phys., 1991, 69: 185 |
| 34 | Wolf D. A broken-bond model for grain boundaries in face-centered cubic metals [J]. J. Appl. Phys., 1990, 68: 3221 |
| 35 | Brokman A, Balluffi R W. Coincidence lattice model for the structure and energy of grain boundaries [J]. Acta Metall., 1981, 29: 1703 |
| 36 | Randle V. The role of the grain boundary plane in cubic polycrystals [J]. Acta Mater., 1998, 46: 1459 |
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