Volume 43 Issue 4
Apr.  2023
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WANG Mafa, LI Junling, LIU Sen. The influence of density gradient of driving gas on projectile launching velocity[J]. Explosion And Shock Waves, 2023, 43(4): 042202. doi: 10.11883/bzycj-2022-0209
Citation: WANG Mafa, LI Junling, LIU Sen. The influence of density gradient of driving gas on projectile launching velocity[J]. Explosion And Shock Waves, 2023, 43(4): 042202. doi: 10.11883/bzycj-2022-0209

The influence of density gradient of driving gas on projectile launching velocity

doi: 10.11883/bzycj-2022-0209
  • Received Date: 2022-05-16
  • Rev Recd Date: 2022-11-01
  • Available Online: 2022-11-02
  • Publish Date: 2023-04-05
  • The most common hypervelocity propulsion systems are light gas guns. Especially, the ability of two-stage light gas guns is suitable to accelerate projectile at velocities ranging from 2 km/s to 9 km/s. However, velocities higher than 10 km/s are demanded eagerly for ballistic limit equations on on-orbit impacts and meteoroids. In order to enhance the launch performance of the light-gas guns, a concept of using density-gradient gas as the driving gas instead of single helium or hydrogen gas has been proposed. An analytical acceleration model of the projectile in the launch tube with constant cross-sectional area is deduced. The launch process can be divided into three stages. The first stage is the projectile driven by the first shock wave. The second stage is the projectile driven by shock waves reflected on the gas interface. The last stage is the projectile caught up by the rarefaction wave created by the suddenly stop of the piston. The comparison in launch performance between neon-helium density-gradient driving gas and helium driving gas is made, and the influences of parameters of the gradient gas on the launch performance are studied. Results show that the neon-helium density-gradient driving gas can improve the launch velocity by about 0.4−1.4 km/s or lower the maximum base pressure by about 0.2−0.9 GPa. The biggest influential factors for the launch velocity and the maximum base pressure are the density of high density gas and the piston velocity, following by the initial gas pressure and the gaseous polytrophic index. High density gas with both high density and high gaseous polytrophic index would be the prior choice due to the reason that higher gaseous polytrophic index could make the maximum base pressure lower. The launch velocity has little correlation with the ratio of high density gas. However, low ratio of high density gas could lower the maximum base pressure.
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  • [1]
    SWIFT H F. Light-gas gun technology: a historical perspective [M]//CHHABILDAS L C, DAVISON L, HORIE Y. High-Pressure Shock Compression of Solids Ⅷ. Berlin: Springer, 2005: 1–35.
    [2]
    LEXOW B, WICKERT M, THOMA K, et al. The extra-large light-gas gun of the fraunhofer EMI: applications for impact cratering research [J]. Meteoritics & Planetary Science, 2013, 48(1): 3–7. DOI: 10.1111/j.1945-5100.2012.01427.x.
    [3]
    HUNEAULT J, LOISEAU J, HIGGINS A J. Coupled lagrangian gasdynamic and structural hydrocode solvers for simulating an implosion-driven hypervelocity launcher [C]//Proceedings of the 51st AIAA Aerospace Sciences Meeting including the New Horizons Forum and Aerospace Exposition. Grapevine: AIAA, 2013: 1–21. DOI: 10.2514/6.2013-274.
    [4]
    HUNEAULT J, LOISEAU J, HILDEBRAND M, et al. Down-bore velocimetry of an explosively driven light-gas gun [J]. Procedia Engineering, 2015, 103: 230–236. DOI: 10.1016/j.proeng.2015.04.031.
    [5]
    HUNEAULT J. Development of an implosion-driven hypervelocity launcher for orbital debris impact simulation [D]. Montreal: McGill University, 2013: 3–10.
    [6]
    MORITOH T, KAWAI N, NAKAMURA K G, et al. Three-stage light-gas gun with a preheating stage [J]. Review of Scientific Instruments, 2004, 75(2): 537–540. DOI: 10.1063/1.1641155.
    [7]
    林俊德, 张向荣, 朱玉荣, 等. 超高速撞击实验的三级压缩气炮技术 [J]. 爆炸与冲击, 2012, 32(5): 483–489. DOI: 10.11883/1001-1455(2012)05-0483-07.

    LIN J D, ZHANG X R, ZHU Y R, et al. The technique of three-stage compressed-gas gun for hypervelocity impact [J]. Explosion and Shock Waves, 2012, 32(5): 483–489. DOI: 10.11883/1001-1455(2012)05-0483-07.
    [8]
    HILDEBRAND M. Concepts for increasing the projectile velocity of an implosion driven launcher [D]. Montreal: McGill University, 2016: 1–2.
    [9]
    CHRISTIANSEN E L. Meteoroid/debris shielding: NASA/TP-2003-210788 [R]. NASA, 2003.
    [10]
    王青松, 王翔, 郝龙, 等. 三级炮超高速发射技术研究进展 [J]. 高压物理学报, 2014, 28(3): 339–345. DOI: 10.11858/gywlxb.2014.03.012.

    WANG Q S, WANG X, HAO L, et al. Progress on hypervelocity launcher techniques using a three-stage gun [J]. Chinese Journal of High Pressure Physics, 2014, 28(3): 339–345. DOI: 10.11858/gywlxb.2014.03.012.
    [11]
    王海福, 冯顺山, 刘有英. 空间碎片导论 [M]. 北京: 科学出版社, 2010: 1–5.
    [12]
    SEIGEL A E. The theory of high speed guns [R]. Paris: Advisory Group for Aerospace Research and Development, 1965.
    [13]
    PUTZAR R, SCHAEFER F. Concept for a new light-gas gun type hypervelocity accelerator [J]. International Journal of Impact Engineering, 2016, 88: 118–124. DOI: 10.1016/j.ijimpeng.2015.09.009.
    [14]
    李维新. 一维不定常流与冲击波 [M]. 北京: 国防工业出版社, 2003: 439–445.
    [15]
    北京工业学院八系《爆炸及其作用》编写组. 爆炸及其作用(上册) [M]. 北京: 国防工业出版社, 1979: 190–195.
    [16]
    Century Dynamics Inc. Autodyn user's manual: version 6.1 [M]. Houston: Century Dynamics Inc., 2005.
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