2021/09/24 by Brenden W. Hamilton, Hamilton, Brenden W., Matthew P. Kroonblawd +3
Chemistry · Earth and Planetary Sciences · Engineering · Materials Science · #Anisotropy #Chemical physics #Chemistry #Classical mechanics #Composite material #Computational chemistry #Crystallography #Detonation #Energetic Materials and Combustion #Energetic material #Energy (signal processing) #Energy profile #Explosive material #FOS: Physical sciences #Geometry #High-Velocity Impact and Material Behavior #High-pressure geophysics and materials #Hotspot (geology) #Internal energy #Kinetic energy #Materials Science (cond-mat.mtrl-sci) #Materials science #Mechanics #Microstructure #Molecular dynamics #Optics #Physics #Potential energy #Projectile #Shock (circulatory) #Shock wave #TATB #Thermodynamics
paper · pdf · doi:10.48550/arxiv.2109.12138
openalex publication_date 2021/09/24 · openalex created_date 2022/07/25 · openalex updated_date 2026/08/05
In energetic materials, the localization of energy into "hotspots" when a shock wave interacts with the material's microstructure is known to dictate the initiation of chemical reactions and detonation. Recent results have shown that, following the shock-induced collapse of pores with circular cross-sections, more energy is localized as internal potential energy (PE) than can be inferred from the kinetic energy (KE) distribution. This leads to a complex thermo-mechanical state that is typically overlooked. The mechanisms associated with pore collapse and hotspot formation and the resulting energy localization are known to be highly dependent on material properties, especially its ability to deform plastically and alleviate strain energy, as well as the size and shape of the pore. Therefore, we use molecular dynamics simulations to characterize shock-induced pore collapse and the subsequent formation of hotspots in TATB, a highly anisotropic molecular crystal, for various defect shapes, shock strengths and crystallographic orientations. We find that the the localization of energy as PE is consistently higher and its extent larger than as localized as KE. A detailed analysis of the MD trajectories reveal the underlying molecular process that govern the effect of orientation and pore shape on the resulting hotspots. We find that the regions of highest PE for a given KE relate to not the impact front of the collapse, but the areas of maximum plastic deformation, while KE is maximized at the point of impact. A comparison with previous results in HMX reveal less energy localization in TATB which could be a contributing factor to its insensitivity.