Calculation model of blast wave loadings of cylindrical charges air moving explosion
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摘要: 为预测战斗部爆炸威力，对柱形装药运动爆炸的入射和反射冲击波峰值超压和最大冲量开展数值仿真研究。首先，基于AUTODYN有限元分析程序提出了“三阶段”的装药运动爆炸有限元分析方法，通过与已有静止和运动爆炸试验结果对比验证了方法的可靠性。然后，考虑装药运动速度、长径比、比例距离、方位角和刚性反射等影响因素开展了运动爆炸工况下200组柱形装药的数值模拟。结果表明：相较于静爆，动爆冲击波场整体前移，波阵面强度在装药运动方向增强而在反方向减弱，该影响与装药运动速度正相关。最后，针对柱形装药空中自由场运动爆炸和垂直于目标迎爆面运动爆炸的典型工况，分别提出了装药运动爆炸入射和反射冲击波峰值超压以及最大冲量的计算模型，该模型与2种战斗部柱形TNT装药运动爆炸工况的数值模拟结果符合良好，能较好地计算柱形装药空中运动爆炸冲击波荷载。Abstract: Ammunition warheads are typically cylindrical charges that detonated at moving stage. To accurately calculating the blast wave power field and the blast loadings acting on the structure of cylindrical charges air moving explosion, the peak overpressure and maximal impulse of the incident and reflected blast waves of the cylindrical charges air moving explosion were numerically simulated. Firstly, a three-stage finite element analysis method for cylindrical charges air moving explosion was proposed based on the AUTODYN finite element analysis program, and the reliability of the method was verified by comparing the simulated and test data of existing charges air static and moving explosion tests. Then, on the basis of considering factors such as charge moving velocity, length to diameter ratio, scaled distance, azimuth angle, and rigid reflection, numerical simulations were conducted for 200 sets of scenarios of the cylindrical charges air moving explosion. The distribution characteristics of the moving explosion blast wave field, incident and reflected blast wave loadings were quantitatively analyzed. The results indicate that the blast wave field of moving explosion is moved forward compared to the static explosion, and the wavefront strength is enhanced in the direction of charge movement and weakened in the opposite direction. The effect is positively correlated with the charge moving velocity, while changing the length to diameter ratio is less affected the blast wave field. Furthermore, for the typical scenarios of cylindrical charges air moving explosion in free field and reflected field where cylindrical charges were perpendicular to the target surface air moving explosion, the calculation models for the peak overpressure and maximal impulse of the incident and reflected blast waves of cylindrical charges air moving explosion were proposed. Finally, through carrying out numerical simulations of 40 sets of scenarios for the moving explosions of two simplified cylindrical TNT charges of prototype warheads, and comparing data of calculation models and simulations, the applicability of the proposed calculation model was validated. The results indicate that the calculation model is good at evaluating the blast wave loading of cylindrical charges air moving explosion, which can also provide a certain reference for predicting the moving explosive power of warheads.
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Key words:
- cylindrical charge /
- air moving explosion /
- peak overpressure /
- maximal impulse /
- calculation model
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图 1 柱形装药空中动爆有限元模型
Figure 1. Finite element model of cylindrical charges air moving explosion
图 2 局部和全域模型中不同网格尺寸下的空气压力时程曲线
Figure 2. Air pressure-time histories corresponding to different mesh sizes in local and global models
图 10 装药运动扰动压力场和有限元模型
Figure 10. The disturbed pressure field of moving charge and finite element model
图 11 不同速度下扰动压力场对入射冲击波超压时程的影响
Figure 11. Influence of the disturbed pressure field on incident overpressure-time histories with different velocities
图 12 不同时刻柱形装药动爆冲击波压力云图（L/D=6, Ma =4）
Figure 12. Instantaneous blast wave pressure contours of cylindrical charges air moving explosion at different times (L/D=6, Ma=4)
图 13 不同装药长径比的冲击波压力云图（Ma =0）
Figure 13. Instantaneous blast wave pressure contours of cylindrical charges air moving explosion with different L/Ds (Ma =0)
图 14 典型比例距离处不同长径比装药的冲击波峰值超压和最大冲量与方位角的关系（Ma =0）
Figure 14. Blast wave peak overpressure and maximal impulse vs azimuth angle of charges with different L/Ds at typical scaled distances (Ma =0)
图 15 不同速度柱形装药的动爆冲击波压力云图（0.1 ms）
Figure 15. Instantaneous blast wave pressure contours of cylindrical charges air moving explosion with different velocities (0.1 ms)
图 17 典型比例距离处的冲击波峰值超压和最大冲量与方位角的关系（L/D=6）
Figure 17. Blast wave peak overpressure and maximal impulse vs azimuth angle of charges with different velocities at typical scaled distances (L/D=6)
图 18 不同运动速度入射冲击波峰值超压（L/D=6）
Figure 18. Peak overpressure of blast wave with different moving velocities (L/D=6)
图 19 典型方位角入射冲击波峰值超压（L/D=6）
Figure 19. Peak overpressure of blast wave under typical azimuth angles (L/D=6)
图 20 不同运动速度入射冲击波最大冲量（L/D=6）
Figure 20. Maximal impulse of blast wave under typical azimuth angles with different moving velocities (L/D=6)
图 21 典型方位角入射冲击波最大冲量（L/D=6）
Figure 21. Maximal impulse of blast wave under typical azimuth angles (L/D=6)
图 23 不同垂直比例距离处的冲击波超压反射系数（L/D=6）
Figure 23. Reflection coefficients of blast overpressure at different vertical scaled distances (L/D=6)
图 24 23 kg装药的动爆冲击波荷载
Figure 24. Blast wave loadings of 23 kg charges air moving explosion
图 25 280 kg装药的动爆冲击波荷载
Figure 25. Blast wave loadings of 280 kg charges air moving explosion
表 1 扰动压力场影响下的入射冲击波峰值超压相对误差
Table 1. Relative deviations of peak incident overpressure influenced by the disturbance pressure field
Ma Z/(m·kg-1/3) δd(%) α=0° α=45° α=90° α=135° α=180° 1 0.3 2.88 0.76 0.97 0.18 9.08 0.4 0.40 0.19 0.03 0.41 6.46 0.5 2.63 0.71 0.42 0.35 2.94 4 0.3 16.41 0.93 7.67 1.40 29.46 0.4 7.75 1.10 4.57 5.15 14.64 0.5 3.66 2.63 2.71 8.14 5.78 
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表 2 峰值超压的拟合系数
Table 2. Coefficients of the fitted formula for peak overpressure
j Aj,1 Aj,2 Aj,3 Aj,4 Aj,5 1 −926 −308 721 −4 236 2 1497 858 −558 26 −559 3 −224 −133 111 −7 70 k A1,k,1 A1,k,2 A1,k,3 A2,k,1 A2,k,2 A2,k,3 A3,k,1 A3,k,2 A3,k,3 1 −2287 −60 1782 2769 250 −1686 −291 −40 182 2 −262 −74 484 −893 212 −205 491 −50 −51 3 −873 39 829 732 −160 −685 −152 50 102 4 −1781 89 1304 1854 −233 −932 −242 47 85
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表 3 比冲量的拟合系数
Table 3. Coefficients of the fitted formula for the scaled impulse
j Bj,1 Bj,2 Bj,3 Bj,4 Bj,5 1 372 214 −148 3 −181 2 −277 −72 108 −2 46 3 40 36 −10 0 −17 k B1,k,1 B1,k2 B1,k,3 B2,k,1 B2,k,2 B2,k,3 B3,k,1 B3,k,2 B3,k,3 1 −74 31 47 28 −26 12 68 6 −40 2 928 7 −740 −1249 −2 743 521 1 −244 3 525 −1 −414 −676 −5 413 267 2 −129 4 74 −2 −49 −270 −8 167 179 3 −87
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