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Study on the Initiation Capacities of Conical Ring Booster Pellets

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Treść / Zawartość
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Warianty tytułu
Języki publikacji
EN
Abstrakty
EN
The insensitive main charge explosive is becoming an important part of modern weapon development. Insensitive main charge explosives generally have a high critical initiation pressure. The detonation pressure of a traditional cylindrical booster pellet is constant at a specific density and consequently has insufficient energy output to reliably initiate an insensitive main charge explosive. To ensure that this requirement could be achieved, the conical ring booster pellet was designed and optimized. Eight-point-synchronous explosive circuits were designed as appropriate to the sizes of the four booster pellets. The initiation processes of the four conical booster pellets equipped with the eight-point circuit were simulated using ANSYS/LY-DYNA software. The experimental measurements were performed in order to test the initiation capacities of these conical booster pellets. The results demonstrated that their initiation capacities are much better than the initiation capacity of a cylindrical booster pellet. The optimum size of the conical ring booster pellet is when the ratio of the inner to the upper diameter is 0.52, the ratio of the inner to the lower diameter is 0.44, and the ratio of the height to the lower diameter is 0.50.
Rocznik
Strony
335--348
Opis fizyczny
Bibliogr. 12 poz., rys., tab.
Twórcy
autor
  • Chemical Industry and Ecology College, North University of China, Taiyuan, Shanxi 030051, P.R. China
autor
  • Chemical Industry and Ecology College, North University of China, Taiyuan, Shanxi 030051, P.R. China
autor
  • Chemical Industry and Ecology College, North University of China, Taiyuan, Shanxi 030051, P.R. China
autor
  • Jinxi industries group Co., Ltd, Taiyuan, Shanxi 030051, P.R. China
Bibliografia
  • [1] Department of Defense Test Method Standard: Hazard Assessment Tests for Non-Nuclear Munitions, MIL-STD-2105B, Department of Defense, 1994.
  • [2] Flegg G.T., Frankl P.J., Griffiths T.T., Explosive Train Scale Shock Testing of New Energetic Materials, QinetiQ, Fort Halstead, Sevenoaks, Kent, TN14 7BP, UK, 2010.
  • [3] Dallman J.C., Measurements of Detonation-Wave Spreading and Local Particle Velocity at the Surface of 17-mm LX-07 Hemispherical Boosters, Report No. LA-11414-MS, Los Alamos National Laboratory, 1988.
  • [4] Spahn P.F., Booster Explosive Ring, US Patent 5233929, 1993.
  • [5] Spahn P.F., Embedded Can Booster, US Patent 5221810, 1993.
  • [6] Hu L.S., Hu S.Q., Cao X., Study on the Initiation Capacities of Two Booster Pellets, Cent. Eur. J. Energ. Mater., 2012, 9(3), 261-272.
  • [7] Lee E.L., Hornig H.C., Kury J.W., Adiabatic Expansion of High Explosive Detonation Products, Report No. UCRL-50422, Lawrence Livermore National Laboratory, Livermore, CA, 1968.
  • [8] Alia A., Souli M., High Explosive Simulation Using Multi-Material Formulations, Appl. Therm. Eng., 2006, 26(10), 1032-1042.
  • [9] Johnson G.R., Cook W.H., Fracture Characteristics of Three Metals Subjected to Various Strains, Strain Rates, Temperatures and Pressures, Eng. Fract. Mech., 1985, 21(1), 31-48.
  • [10] Li Y., Experiment of Booster Shock Initiation and Its Numerical Simulation (In Chinese), North University of China, China, 2010.
  • [11] Walker F.E., Wasley R.J., Critical Energy for Shock Initiation of Heterogeneous Explosives, Explosivstoffe, 1969, 17(1), 9-13.
  • [12] Zhang S.Z., Explosion Principle (in Chinese), National Defense Industry Press, Beijing, 2005, pp. 394-397.
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-739b0cec-565b-4321-8596-16601d6692c8
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