Coupled model for grain rotation, dislocation plasticity and grain boundary sliding in fine-grained solids

被引:35
作者
Borodin, E. N. [1 ]
Mayer, A. E. [2 ,3 ]
Gutkin, M. Yu [4 ,5 ,6 ]
机构
[1] Univ Manchester, Dept MACE, Mech & Phys Solids Res Grp, Manchester M13 9PL, Lancs, England
[2] Chelyabinsk State Univ, Dept Phys, Br Kashirinykh Str 129, Chelyabinsk 454001, Russia
[3] South Ural State Univ, Lab Funct Mat, Natl Res Univ, Lenin Prospect 76, Chelyabinsk 454080, Russia
[4] Inst Problems Mech Engn RAS, VO, Bolshoj Pr 61, St Petersburg 199178, Russia
[5] ITMO Univ, Kronverkskiy Pr 49, St Petersburg 197101, Russia
[6] Peter Great St Petersburg Polytech Univ, Dept Mech & Control Proc, Polytekhnicheskaya 29, St Petersburg 195251, Russia
关键词
Nanocrystalline solids; Grain rotation; Dislocation plasticity; Grain boundary sliding; High-strain-rate deformation; Structural models of plasticity; Numerical simulations; YIELD-STRESS; NANOCRYSTALLINE MATERIALS; MICROSTRUCTURAL EVOLUTION; DEFORMATION MECHANISMS; ATOMISTIC SIMULATIONS; MOLECULAR-DYNAMICS; EDGE DISLOCATION; STRAIN-RATE; BEHAVIOR; COPPER;
D O I
10.1016/j.ijplas.2020.102776
中图分类号
TH [机械、仪表工业];
学科分类号
0802 ;
摘要
Based on a new model coupling both direct and inverse grain rotation processes, we discuss interrelations between the dislocation mechanism of plasticity and the grain boundary sliding in fine-grained solids. The high-strain-rate deformation conditions, corresponding to molecular dynamics simulations, and processes of severe plastic deformation are in the focus of our consideration. The model correctly predicts the transition point below which the shape of nanograins remains equiaxed after deformation. For nanocrystalline copper, it corresponds to grains of several nanometers in size, while for ultrafine-grained copper - some hundreds of nanometers, that is in a good agreement with experimental data. A consequence from the existence of two transition points is the presence of grain size range between these points where the grains remain distorted after deformation. Our calculations show that for copper, this range is from 6 to 20 nm. The model also predicts the existence of a limit strain rate above which grains cannot be equiaxed. For this strain rate, our calculations give tens of inverse seconds for nanocrystalline copper and a few inverse seconds for ultrafine-grained one.
引用
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页数:19
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