Deformation twinning-induced texture evolution in Ti under shock compression: An atomistic simulation study

Y Y. T. Chen (State Key Laboratory of Precision Space-time Information Sensing Technology, Department of Precision Instrument, Tsinghua University 1 , Beijing 100084,) S S. C. Hu (China Nuclear Power Operation Technology Corporation, LTD 2 , Wuhan, Hubei,) L L. Wang L L. Lu (Key Laboratory of Advanced Technologies of Materials, Ministry of Education, and Dynamic Materials Data Science Center, Southwest Jiaotong University 3 , Chengdu, Sichuan,) N N. B. Zhang (Key Laboratory of Advanced Technologies of Materials, Ministry of Education, and Dynamic Materials Data Science Center, Southwest Jiaotong University 3 , Chengdu, Sichuan,) Y Y. Cai S S. N. Luo (Key Laboratory of Advanced Technologies of Materials, Ministry of Education, and Dynamic Materials Data Science Center, Southwest Jiaotong University 3 , Chengdu, Sichuan,)

Abstract

Shock-induced texture evolution in polycrystalline titanium (Ti) with different initial textures under different impact velocities is investigated systematically via large-scale molecular dynamics simulations. {101¯2}⟨101¯1⟩, {101¯1}⟨101¯2⟩, and {112¯1}⟨112¯6¯⟩ deformation twinning are observed upon shock compression; however, the texture evolution is mainly attributed to {101¯2} and {101¯1} twinning based on resolved shear stress analysis and orientation mapping. When a single-step texture change occurs in the loading configuration, the {101¯1} twinning dominates, whereas when a two-step texture change occurs in the loading configuration, the {101¯2} twinning prevails: a new texture is initially induced via the {101¯2} twinning, followed by the formation of another texture component through the {101¯1} twinning, except for the loading configuration initially with no texture. The twinning dislocations of {112¯1} twins comprise both an edge component and a screw component. The {101¯2} and {101¯1} twinning occur via the HCPmatrix to BCC to HCPtwin phase transformation sequence, induced solely by atomic shuffles without shear deformation. The HCP phase and the transient BCC phase obey the Pitsch–Schrader orientation relationship. Different twinning relationships can be achieved by different variants during phase transformation.

Article Details

Volume / Issue Vol. 138, Issue 2
Published July 14, 2025
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (7)

Y

Y. T. Chen

State Key Laboratory of Precision Space-time Information Sensing Technology, Department of Precision Instrument, Tsinghua University 1 , Beijing 100084,

S

S. C. Hu

China Nuclear Power Operation Technology Corporation, LTD 2 , Wuhan, Hubei,

L

L. Wang

L

L. Lu

Key Laboratory of Advanced Technologies of Materials, Ministry of Education, and Dynamic Materials Data Science Center, Southwest Jiaotong University 3 , Chengdu, Sichuan,

N

N. B. Zhang

Key Laboratory of Advanced Technologies of Materials, Ministry of Education, and Dynamic Materials Data Science Center, Southwest Jiaotong University 3 , Chengdu, Sichuan,

Y

Y. Cai

S

S. N. Luo

Key Laboratory of Advanced Technologies of Materials, Ministry of Education, and Dynamic Materials Data Science Center, Southwest Jiaotong University 3 , Chengdu, Sichuan,