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AIR BLAST CAUSED BY HYPERVELOCITY IMPACT

机译:高速冲击造成的空气冲击

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An experimental, analytical, and numerical investigation was conducted to measure air pressure at ambient conditions on the target surface near the point of normal impact into semi-infinite rolled homogeneous armor (RHA) of a high-speed, 3/8-inch diameter tungsten carbide sphere launched from a two-stage light gas gun. Numerical simulations of the impact using CTH were also conducted in which the crater lip and ejecta motion were successfully coupled with the surrounding air. Impact speeds varied from 0.9 to 3.8 km/s. In addition to modeling the blast using the CTH code, an analytical model of the air blast field resulting from the impact has been developed employing the blast generated by a small explosive charge initiated at the time and point of impact. This is a one-dimensional solution in which all characteristics of the blast field are a function only of the radius from the charge center and the energy released by the charge. Thus, a single, empirically derived parameter, the equivalent explosive charge energy, completely defines the blast field. For each test, this parameter was obtained from a least squares fit to the peak pressures measured as a function of distance from the impact (explosion) center. The model predicts the data well at all test speeds. The tests, accompanying modeling, and CTH calculations resulted in the following conclusions: The air blast field contains about 0.7 % of the kinetic energy of the impacting projectile and results from three sources: (1) the air entrained by fee projectile and impinging the target plate; (2) the air accelerated by the radially expanding crater lip; and (3) the air entrained by the ejecta.
机译:进行了实验,分析和数值研究,以测量环境条件下目标表面上法向冲击点附近的空气压力,该压力作用于高速3/8英寸直径的半无限滚动均质装甲(RHA)中由两级轻气枪发射的硬质合金球。还使用CTH对撞击进行了数值模拟,其中火山口和弹射运动已与周围空气成功耦合。撞击速度从0.9到3.8 km / s不等。除了使用CTH代码对爆炸进行建模外,还开发了使用冲击时爆炸点所产生的爆炸所产生的冲击力,从而建立了由冲击产生的爆炸场的分析模型。这是一维解决方案,其中爆炸场的所有特征仅是距装药中心的半径和装药释放的能量的函数。因此,一个凭经验得出的参数即等效炸药装料能量完全定义了爆炸场。对于每个测试,该参数是从与所测得的峰值压力的最小二乘拟合获得的,该峰值压力是距撞击(爆炸)中心的距离的函数。该模型在所有测试速度下都能很好地预测数据。测试,伴随的建模和CTH计算得出以下结论:爆炸场包含约0.7%的撞击弹丸动能,并来自以下三个方面:(1)费用弹丸夹带并撞击目标的空气盘子; (2)由径向扩展的火山口唇加速的空气; (3)喷射器夹带的空气。

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