Volume 40 Issue 5
May  2020
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WANG Tao, WANG Bing, LIN Jianyu, ZHONG Min, BAI Jingsong, LI Ping, TAO Gang. Numerical investigations of the interface instabilities of metallic material under implosion in cylindrical convergent geometry[J]. Explosion And Shock Waves, 2020, 40(5): 052201. doi: 10.11883/bzycj-2019-0150
Citation: WANG Tao, WANG Bing, LIN Jianyu, ZHONG Min, BAI Jingsong, LI Ping, TAO Gang. Numerical investigations of the interface instabilities of metallic material under implosion in cylindrical convergent geometry[J]. Explosion And Shock Waves, 2020, 40(5): 052201. doi: 10.11883/bzycj-2019-0150

Numerical investigations of the interface instabilities of metallic material under implosion in cylindrical convergent geometry

doi: 10.11883/bzycj-2019-0150
  • Received Date: 2019-04-23
  • Rev Recd Date: 2019-07-21
  • Publish Date: 2020-05-01
  • In this paper, the dynamical behavior of metal interface instability driven by implosion in cylindrical convergent geometry is numerically investigated by using an in-house high-fidelity detonation and shock wave program. The results indicate that, in the development process of perturbed interface, the RM instability is primary from the initial shock to 12 μs; after 12 μs and before rebound loading of the convergent shock wave, the interface moves towards the center deceleratedly with an increasing acceleration, and the RT instability dominates the evolution of perturbed interface; after the re-shock, the perturbation growth is dominated by the RM instability again. The effects of initial conditions such as the initial amplitude, wavelength (mode number), thickness of steel shell and geometry configuration on the metal interface instability driven by cylindrical implosion are also investigated. It is shown that, the instantaneous amplitude is larger when the initial amplitude is larger; the instantaneous amplitude is smaller when the initial wavelength is smaller, and a cutoff wavelength exists; the larger thickness of steel shell can suppress the perturbation growth, and a cutoff thickness also exists; the geometrical convergent effect causes the perturbation to grow faster.
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