Experiments and numerical simulations of plate gap model for high energetic materials

18th APS-SCCM; 24th AIRAPT

Kubota, S.^1 ; Saburi, T.^1 ; Ogata, Y.^1 ; Wada, Y.^1 ; Nagayama, K.^2

National Institute of Advanced Industrial Science and Technology, 16-1 Onogawa, Ibaraki, Tsukuba

305-8569, Japan^1

Kyushu University, Motooka 744, Nishi-ku, Fukuoka

819-0395, Japan^2

关键词: Calculation results;    Detonation propagation;    Experimental and numerical studies;    Extraction of information;    High energy materials;    Numerical procedures;    Shock to detonation transitions;    Theoretical maximum densities;   

Others  :  https://iopscience.iop.org/article/10.1088/1742-6596/500/5/052022/pdf
DOI  :  10.1088/1742-6596/500/5/052022

来源: IOP

【 摘 要 】

Experimental and numerical study for detonation propagation was conducted using the system in which the high energy materials and air gaps alternately stacked. The aim of this simulation is an extraction of information of the EOS for detonation product at arbitrary initial density from the numerical simulation with EOS at TMD (theoretical maximum density). In this report, we described the numerical procedure and an example of the calculation result. On the other hand, the experiment was designed for confirmation of the validity of our reactive flow simulation. The experimental system for this study consists of the pellet explosives and PMMA rings, PMMA pipe and booster explosive part. The pellets and the rings were alternately stacked in the PMMA pipe to make the system. The diameter of the pellet was 20 mm and the thicknesses were 10 or 5 mm. The thickness of the ring was varied to adjust the size of the air gaps between the pellets. The sample explosive was a composition A5 (RDX 98.8 wt%). The relationship between the bulk density which was estimated by the thicknesses of the pellets and the air gaps and the average detonation velocity was compared with the data for RDX. The slopes of those relationships differed mutually. Although the experimental results can be used for confirmation of the validity of the numerical procedure, it does not simulate the detonation wave in the powdered explosive. It may show the interesting process that consists of the shock wave in air, shock to detonation transition and steady detonation.