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The present study examines the role of transverse waves and hydrodynamic instabilities mainly, Richtmyer–Meshkov instability (RMI) and Kelvin–Helmholtz instability (KHI) in detonation structure using two-dimensional high-resolution numerical simulations of Euler equations. To compare the numerical results with those of experiments, Navier–Stokes simulations are also performed by utilizing the effect of diffusion in highly irregular detonations. Results for both moderate and low activation energy mixtures reveal that upon collision of two triple points a pair of forward and backward facing jets is formed. As the jets spread, they undergo Richtmyer–Meshkov instability. The drastic growth of the forward jet found to have profound role in re-acceleration of the detonation wave at the end of a detonation cell cycle. For irregular detonations, the transverse waves found to have substantial role in propagation mechanism of such detonations. In regular detonations, the lead shock ignites all the gases passing through it, hence, the transverse waves and hydrodynamic instabilities do not play crucial role in propagation mechanism of such regular detonations. In comparison with previous numerical simulations present simulation using single-step kinetics shows a distinct keystone-shaped region at the end of the detonation cell.  相似文献   
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INTRODUCTIONVarious geometrical configurations havebeen used to obtain an understanding of phenom-ena in accelerated inhomogeneous flows( aifs) ,e.g. Richtmyer- Meshkov ( RM) and Rayleigh-Taylor( RT) flows,where visiometrics are beingemphasized more and more by the community[1] .The classical configuration,an acceleration orimpulse directed perpendicular to a planar inter-face between fluids of different density perturbedby a small- amplitude sinusoid has attracted muchattention for evo…  相似文献   
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