2017/09/26 by N. N. Myagkov · 1 citation
Engineering · Materials Science · Physics and Astronomy · #Distribution function #Explosive material #Exponent #Fluid Dynamics Simulations and Interactions #Fragmentation (computing) #High-Velocity Impact and Material Behavior #Particle Dynamics in Fluid Flows #Projectile #Scaling #Shield #cond-mat.mtrl-sci #cond-mat.soft #physics.app-ph
paper · pdf · doi:10.1134/s1063776117120068
published in Journal of Experimental and Theoretical Physics 126(1), 50-63 (Pleiades Publishing) · 25 pages, 16 figures
arxiv created 2017/09/26 · openalex created_date 2017/10/06 · openalex publication_date 2018/01/01 · arxiv updated 2018/03/12 · openalex updated_date 2026/08/05
In this paper, we consider the problem of the fragmentation of an aluminum projectile on a thin steel mesh shield at high-velocity impact in a three-dimensional (3D) setting. The numerical simulations are carried out by the smoothed particle hydrodynamics method applied to the equations of mechanics of deformable solids. Quantitative characteristics of the projectile fragmentation are obtained by studying statistics of the cloud of fragments. Considerable attention is given to scaling laws accompanying the fragmentation of the projectile. Scaling is carried out using the parameter K , which defines the number of the mesh cells in the projectile diameter. It is found that the dependence of the critical velocity V c of fragmentation on the parameter K consists of two branches that correspond to two modes of the projectile fragmentation associated with the “small” and “large” aperture of the mesh cell. We obtain the dependences of the critical velocity V c on the projectile diameter and the mesh parameters for both modes of the fragmentation. It is shown that the average cumulative mass distributions constructed at V c exhibit the property of scale invariance, splitting into two groups of distributions corresponding exactly to the modes of the projectile fragmentation. In each group, the average cumulative distributions show good coincidence in the entire mass region; moreover, in the intermediate mass region, each group of distributions has a power-law distribution with an exponent τ different from that in the other group. Conclusions about the dependence of the exponent of the power-law distribution τ on the fragmentation mode are made.