journal article·2016-08Open access

Twin boundary activated α → ω phase transformation in titanium under shock compression

Hongxiang Zong, Xiangdong Ding, Turab Lookman, Jun Sun

Acta Materialia· Volume 115

Abstract

Abstract The role of grain boundary structures on the shock response of hexagonal-close-packed (hcp) metals is little understood. We use molecular dynamics simulations to investigate deformation mechanisms in shock compressed Ti bicrystals with three types of grain boundary (GB) microstructure. Our results show the shock response of phase Ti polycrystals are influenced by the GB characteristics, i.e., elastic shock wave induced inelastic deformation occurs on both sides of the { 10 1 ¯ 2 } coherent twin boundaries (CTBs) but only on one-side of the symmetric incoherent twin boundaries (ITB) or { 1 2 ¯ 10 } tilt grain boundaries regions. In particular, we find that the elastic shock wave can readily trigger the α→ω transformation at { 10 1 ¯ 2 } CTBs but not the other two GBs, and the α→ω transformation at CTBs leads to considerable wave attenuation (i.e., the elastic precursor decay). Combined with first principle calculations, we find that CTBs can facilitate the overcoming of the energy barrier for the α→ω transformation. Our findings have the potential to influence interface engineering and materials design under extreme conditions.
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Research context

OpenAlex topics: High-Velocity Impact and Material Behavior · Microstructure and mechanical properties · High-pressure geophysics and materials

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References (42)

Show source-provided references
1. Chapter 89 dislocations in shock compression and release
2. Effect of loading direction on grain boundary failure under shock loading10.1016/j.actamat.2013.11.026 ↗
3. Shocked materials at the intersection of experiment and simulation10.1007/s10820-008-9107-z ↗
4. The use of shock-structure methods for evaluating high-pressure material properties10.1016/S0734-743X(97)87478-7 ↗
5. On the shock response of cubic metals10.1063/1.3218758 ↗
6. Coupling between plasticity and phase transition of polycrystalline iron under shock compressions10.1016/j.ijplas.2015.01.002 ↗
7. The shock and spall response of three industrially important hexagonal close-packed metals: magnesium, titanium and zirconium10.1098/rsta.2013.0204 ↗
8. Concurrent grain boundary motion and grain rotation under an applied stress10.1016/j.actamat.2011.05.042 ↗
9. Coupling grain boundary motion to shear deformation10.1016/j.actamat.2006.08.004 ↗
10. Grain rotation mediated by grain boundary dislocations in nanocrystalline platinum10.1038/ncomms5402 ↗
11. The disconnection mechanism of coupled migration and shear at grain boundaries10.1016/j.actamat.2012.01.001 ↗
12. Hall–Petch relation and boundary strengthening10.1016/j.scriptamat.2004.06.002 ↗
13. Dynamic plasticity and failure of high-purity alumina under shock loading10.1038/nmat1689 ↗
14. In situ x-ray diffraction measurements of the c/a ratio in the high-pressure epsilon phase of shock-compressed polycrystalline iron10.1103/PhysRevB.83.144114 ↗
15. Shock waves in polycrystalline iron: plasticity and phase transitions10.1103/PhysRevB.89.140102 ↗
16. Ultrahigh strength in nanocrystalline materials under shock loading10.1126/science.1116723 ↗
17. Spall fracture: methodological aspects, mechanisms and governing factors10.1007/s10704-009-9438-0 ↗
18. The influence of phase and substructural evolution during dynamic loading on subsequent mechanical properties of zirconium10.1016/j.actamat.2013.09.009 ↗
19. Loss of shear-strength in polycrystalline tungsten under shock compression10.1063/1.322368 ↗
20. Modeling void growth in polycrystalline materials10.1016/j.actamat.2013.08.004 ↗
21. Differences in deformation behavior of bicrystalline Cu micropillars containing a twin boundary or a large-angle grain boundary10.1016/j.actamat.2014.04.022 ↗
22. Experimental observations of stress-driven grain boundary migration10.1126/science.1178226 ↗
23. Uniaxial stress-driven coupled grain boundary motion in hexagonal close-packed metals: a molecular dynamics study10.1016/j.actamat.2014.09.010 ↗
24. Grain boundary kinetics—II. In situ observations of the role of grain boundary dislocations in high-angle boundary migration10.1016/0001-6160(89)90034-5 ↗
25. Strengthening materials by engineering coherent internal boundaries at the nanoscale10.1126/science.1159610 ↗
26. Ultra-strength materials10.1016/j.pmatsci.2010.04.001 ↗
27. Fast parallel algorithms for short-range molecular-dynamics10.1006/jcph.1995.1039 ↗
28. Collective nature of plasticity in mediating phase transformation under shock compression10.1103/PhysRevB.89.220101 ↗
29. Anisotropic shock response of titanium: reorientation and transformation mechanisms10.1016/j.actamat.2013.11.047 ↗
30. Highly optimized empirical potential model of silicon10.1088/0965-0393/8/6/305 ↗
31. Classical potential describes martensitic phase transformations between the α, β, and ω titanium phases10.1103/PhysRevB.78.054121 ↗
32. Applications of local crystal structure measures in experiment and simulation10.1103/PhysRevB.73.054104 ↗
33. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set10.1103/PhysRevB.54.11169 ↗
34. A generalized solid-state nudged elastic band method10.1063/1.3684549 ↗
35. Atoms, molecules, solids, and surfaces: applications of the generalized gradient approximation for exchange and correlation10.1103/PhysRevB.46.6671 ↗
36. Deformation-induced localized solid-state amorphization in nanocrystalline nickel10.1038/srep00493 ↗
37. Dislocation locking versus easy glide in titanium and zirconium10.1038/nmat4340 ↗
38. Anomalous basal slip activity in zirconium under high-strain deformation10.1080/21663831.2013.794375 ↗
39. Twinning-like lattice reorientation without a crystallographic twinning plane10.1038/ncomms4297 ↗
40. Orientation relations during the α-ω phase transition of zirconium: in situ texture observations at high pressure and temperature10.1103/PhysRevLett.111.195701 ↗
41. New mechanism for the α to ω martensitic transformation in pure titanium10.1103/PhysRevLett.91.025701 ↗
42. Microscopic and crystallographic aspects of retained ω-phase in shock-loaded zirconium and its formation mechanism10.1080/01418619508244356 ↗