考虑形状分布特性的聚能射流侵彻作用规律研究

Study on Penetration Law of Shaped Charge Jet Considering Shape Distribution Characteristics

  • 摘要: 聚能射流对带壳装药的冲击引爆能力与其侵彻有限厚靶板的剩余头部参量及剩余动能密切相关. 为研究考虑形状分布特性的聚能射流侵彻作用规律,建立了聚能射流侵彻靶板及靶后参量计算模型. 开展了50 mm聚能射流成型X光试验及静破甲试验研究,验证了计算模型的可靠性. 在此基础上,计算分析了射流形状、靶板厚度、炸高等因素对聚能射流侵彻有限厚靶板剩余射流头部参量及剩余动能的影响规律. 结果表明:随着靶板厚度的增大,剩余头部参量减小. 随着炸高的增大,一次函数形状射流剩余头部参量持续降低,常函数、二次函数形状的射流剩余头部参量先增大后减小. 在不同的靶板厚度及炸高条件下常函数形状射流的剩余头部参量均为最大;在侵彻有限厚靶板剩余射流动能方面,其剩余射流动能随着靶板厚度的增大而减小. 随着炸高的增大,常函数形状射流剩余动能持续降低,一次、二次函数形状的射流剩余动能先减小后增大. 当炸高小于4~5倍装药口径时,二次函数形状射流剩余能量最高,当炸高大于4~5倍装药口径时,常函数形状聚能射流剩余能量最高.

     

    Abstract: The initiation ability of shaped charge jet on shelled charge is closely related to the residual head parameters and kinetic energy of penetrated finite thickness target. In order to study the penetration law of shaped charge jet , considering the shape characteristics, some calculation models were established for the parameter calculation of shaped charge jet penetrating target plate and parameter calculation of residual head parameters and residual kinetic energy after jet penetration. X-ray test and DOP test of 50 mm shaped charge jet were carried out to verify the reliability of the calculation models. On this basis, the influence of jet shape, target thickness and standoff on the residual jet head parameters and residual kinetic energy was analyzed for shaped charge jet penetrating finite thickness target plate. The results show that with the increase of the thickness of the target, the remaining head parameters decrease. With the increase of the standoff, the residual head parameters of the primary function shaped jet show a decreasing trend, and the residual head parameters of the constant function and quadratic function shaped jet increase first and then decrease. The residual head parameters of the constant function shape jet always show the largest under different target thickness and standoff conditions. In the aspect of jet residual kinetic energy in penetrating finite thickness target, the jet residual kinetic energy decreases with the increase of target thickness. With the increase of the standoff height, the residual kinetic energy of the constant function shaped jet continues to decrease, and the residual kinetic energy of the primary and secondary function shaped jet decreases first and then increases. When the standoff is less than 4~5 times of charge diameter, the residual energy of the quadratic function shaped jet is the highest. When the standoff is greater than 4~5 times of charge diameter, the residual energy of the constant function shaped jet is the highest.

     

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