J. Mater. Sci. Technol. ›› 2025, Vol. 224: 105-124.DOI: 10.1016/j.jmst.2024.10.041

• Research Article • Previous Articles     Next Articles

Shock consolidation and spallation in nanopowdered Mg: Contributed by deformation twinning and disordering

M.Y. Wanga, D.B. Hea,b, W.B. Bic, M. Shanga, Y. Caib, L. Denga, X.M. Zhanga, F. Zhaod,e, J.F. Tanga,*, L. Wanga,b,*   

  1. aCollege of Science, Hunan Agricultural University, Changsha 410128, China;
    bThe Peac Institute of Multiscale Sciences, Chengdu 610207, China;
    cLaboratoroy of Computational Physics, Institute of Applied Physics and Computational Mathematics, Beijing 100088, China;
    dInstitute for Advanced Study, Chengdu University, Chengdu 610106, China;
    eInstitute for Advanced Materials Deformation and Damage from Multiscale, Chengdu University, Chengdu 610106, China
  • Received:2024-09-14 Revised:2024-10-22 Accepted:2024-10-25 Published:2025-07-20 Online:2024-12-04
  • Contact: *E-mail addresses: jftang@hunau.edu.cn (J.F. Tang), wangliang@pims.ac.cn (L. Wang)

Abstract: Nanopowder consolidation under high strain rate shock compression is a potential method for synthesizing and processing bulk nanomaterials, and a thorough investigation of the deformation and its underlying mechanisms in consolidation is of great engineering significance. We conduct non-equilibrium molecular dynamics (NEMD) simulation and X-ray diffraction (XRD) simulation to systematically study shock-induced deformation and the corresponding mechanisms during the consolidation of nanopowdered Mg (NP-Mg). Two different deformation modes govern the shock consolidation in NP-Mg, i.e., deformation twinning at up ≤ 1.5 km s-1 and structural disordering, at up ≥ 2.0 km s-1. They accelerate the collapse of nanopores and void compaction, giving rise to the final consolidation of NP-Mg. Three types of deformation twinning are emitted in NP-Mg, i.e., the extension twinning for {11$\overline{2}$1}〈$\overline{1}$$\overline{1}$26〉, and {1$\overline{1}$02}〈1$\overline{1}$01〉, and the compression {11$\overline{2}$2}〈$\overline{1}$$\overline{1}$23〉 twinning. They are prompted via coupling atomic shuffles and slips. Deformation twinning prefers to occur within the grains as shock along 〈11$\overline{2}$0〉 or its approaching direction (A- and B-type grains), originated from the high-angle grain boundaries (HAGB) at compression stage. They are inhibited within the ones as shocking along 〈0001〉 and the approaching ones (C- and D- type grains). The release and tension loading facilitates the reversible and irreversible detwinning, for the extension and compression twinning, respectively, within the A- and B-type grains. It also contributes to a compression-tension asymmetry for twinning, i.e., release and tension induced extension twinning within the C- and D-type grains. The subsequent spallation is mediated by GB sliding and GB-induced stacking faults at up ≤ 1.5 km s-1, and structural disordering at up ≥ 2.0 km s-1.

Key words: Non-equilibrium molecular dynamics, Nanopowder Mg, Shock consolidation, Deformation twinning, X-ray diffraction