Atomic diffusion, segregation, and grain boundary migration in nickel-based alloys from molecular dynamics simulations

被引:15
|
作者
Simonnin, Pauline [1 ]
Schreiber, Daniel K. [2 ]
Uberuaga, Blas P. [3 ]
Rosso, Kevin M. [1 ]
机构
[1] Pacific Northwest Natl Lab, Phys & Computat Sci Directorate, Richland, WA 99352 USA
[2] Pacific Northwest Natl Lab, Energy & Environm Directorate, Richland, WA 99352 USA
[3] Los Alamos Natl Lab, Mat Sci & Technol Div, Los Alamos, NM 87545 USA
来源
MATERIALS TODAY COMMUNICATIONS | 2023年 / 35卷
关键词
Molecular dynamics; Alloys; Diffusion; Segregation; Grain boundary migration; SELF-DIFFUSION; NI-CR; INTERGRANULAR OXIDATION; INTERSTITIAL DIFFUSION; SOLID-SOLUTIONS; DRIVING-FORCE; FCC; CU; DISLOCATIONS; MECHANISM;
D O I
10.1016/j.mtcomm.2023.105768
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Grain boundary diffusion and metal mobility in alloys control material performance in many applications and yet remain poorly understood at a mechanistic level. With advances in accessible time and length scales for computational molecular simulations, and recent force field developments, we now possess tools to help unravel those mechanisms. Using large-scale molecular dynamics simulations, here we examined vacancy-mediated diffusion processes in Ni-5Cr alloy with low and high-energy grain boundaries. We show that atomic diffusion inside the grain boundary plane is about four times higher than bulk diffusion, at any temperature, and exhibits a typical Arrhenius behavior with a very small energy barrier (similar to 0.8 eV for Cr and 0.7 eV for Ni within 1300-1600 K). Additionally, the fastest diffusing species inverts; Cr diffusion was faster than Ni in the bulk but slower in the grain boundaries. This is attributed to the creation of high cohesive energy clusters of Cr at the grain boundary. Grain boundary migration was also observed to be temperature dependent and appears to be two times higher in the 5% Cr alloy than in pure Ni, highlighting the important role of the alloying element on grain boundary motion.
引用
收藏
页数:11
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