Modeling the microstructural evolution of metallic polycrystalline materials under localization conditions

被引:87
作者
Bronkhorst, C. A. [1 ]
Hansen, B. L.
Cerreta, E. K.
Bingert, J. F.
机构
[1] Los Alamos Natl Lab, Div Theoret, Los Alamos, NM 87545 USA
[2] Los Alamos Natl Lab, Div Mat Sci & Technol, Los Alamos, NM 87545 USA
[3] CALTECH, Grad Aeronaut Labs, Pasadena, CA 91125 USA
关键词
shear localization; microstructure; polycrystal plasticity; dynamic loading; deformation statistics;
D O I
10.1016/j.jmps.2007.03.019
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
In general, the shear localization process involves initiation and growth. Initiation is expected to be a stochastic process in material space where anisotropy in the elastic-plastic behavior of single crystals and inter-crystalline interactions serve to form natural perturbations to the material's local stability. A hat-shaped sample geometry was used to study shear localization growth. It is an axisymmetric sample with an upper "hat" portion and a lower' "brim" portion with the shear zone located between the hat and brim. The shear zone length was 870-890 pm with deformation imposed through a Split-Hopkinson Pressure Bar system at maximum top-to-bottom velocity in the range of 8-25 m/s. The deformation behavior of tantalum tophat samples is modeled through direct polycrystal simulations. An embedded Voronoi-tessellated two-dimensional microstructure is used to represent the material within the shear zone of the sample. A thermo-mechanically coupled elastoviscoplastic single crystal model is presented and used to represent the response of the grains within the aggregate shear zone. In the shoulder regions away from the shear zone where strain levels remain on the order of 0.05, the material is represented by an isotropic J(2) flow theory based upon the elastoviscoplastic Mechanical Threshold Stress (MTS) model for flow strength. The top surface stress versus displacement results were compared to those of the experiments and over-all the simulated stress magnitude is over-predicted. It is believed that the reason for this is that the simulations are two-dimensional. A region within the numerical shear zone was isolated for statistical examination. The vonMises stress state within this isolated shear zone region suggests an approximate normal distribution with a factor of two difference between the minimum and maximum points in the distribution. The equivalent plastic strain distribution within this same region has values ranging between 0.4 and 1.5 and is not symmetric. Other material state distributions are also given. The crystallographic texture within this isolated shear zone is also compared to the experimental texture and found to match reasonably well considering the simulations are two-dimensional. Published by Elsevier Ltd.
引用
收藏
页码:2351 / 2383
页数:33
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