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1. 南京理工大学 机械工程学院, 江苏 南京 210094
2. 军事科学院 国防工程研究院, 北京 100850
Received:06 September 2023,
Published Online:03 January 2024,
Published:08 December 2023
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Wenjun YU, Shengyun CHEN, Shuxin DENG, et al. Numerical Simulation of the Propagation Law of Explosion Shock Wave in Turning Tunnel[J]. Acta Armamentarii, 2023, 44(S1): 180-188.
Wenjun YU, Shengyun CHEN, Shuxin DENG, et al. Numerical Simulation of the Propagation Law of Explosion Shock Wave in Turning Tunnel[J]. Acta Armamentarii, 2023, 44(S1): 180-188. DOI: 10.12382/bgxb.2023.0889.
基于LS-DYNA软件对单次变向通道内
TNT爆炸进行模拟以验证利用LS-DYNA模拟的准确性
研究了变向角度
θ
和曲率半径
R
对变向通道内冲击波传播规律的影响。研究结果表明
当
θ
和
R
较小时
θ
和
R
的变化对通道变向处冲击波参数的变化影响较大
对于远场处的影响较小;当
θ
为90°、
R
为0mm时
通道内变向处外壁面所受压力是内壁面所受压力的2.17倍;随着
θ
的增大
反射冲击波超压峰值减小
冲击波能量分配趋于变向后通道
远场处超压峰值先减小后增大;随着
R
的增加
冲击波在变向处的反射现象不明显
反射冲击波的超压峰值低;随着
θ
和
R
的增加
外壁面与内壁面所受反射压力超压峰值之差减小;当
θ
和
R
分别增加到一定程度时
改变
θ
和
R
对整个通道内冲击波参数变化的影响并不明显
但外壁面压力仍然略高于内壁面压力。
Based on the LS-DYNA software
a single TNT explosion in a turning tunnel is simulated to verify the accuracy of the simulation using LS-DYNA
and the effects of the variable angle
θ
and the radius of curvature
R
on the propagation law of shock wave in the turning tunnel are studied. The results show that
when
θ
and
R
are small
the changes of
θ
and
R
have a greater effect on the changes of shock wave parameters at the tunnel deflection
and the effect is smaller at the far field; when
θ
is 90° and
R
is 0mm
the pressure on the outer wall surface at the deflection in the tunnel is 2.17 times of the pressure on the inner wall surface. With the increase of
θ
the peak overpressure of the reflected shock wave decreases
and the energy distribution of the shock wave tends to change to the back tunnel
and the peak overpressure at the far field decreases first and then increases; with the increase of
R
the reflection phenomenon of the shock wave at the change of direction is not obvious
and the peak overpressure of the reflected shock wave is low; and with the increase of
θ
and
R
the difference between the peak overpressures of th
e reflected pressures received by the outer wall surface and the inner wall surface decreases. When
θ
and
R
are increased to a certain degree
respectively
the effect of changing
θ
and
R
on the change of shock wave parameters in the whole tunnel is not obvious
but the pressure on the outer wall surface is still slightly higher than that on the inner wall surface.
汪泉 , 陆军伟 , 李志敏 , 等 . 负压条件下柱形爆炸罐内爆炸波传播规律 [J ] . 兵工学报 , 2021 , 42 ( 6 ): 1250 - 1256 . DOI: 10.3969/j.issn.1000-1093.2021.06.015 http://doi.org/10.3969/j.issn.1000-1093.2021.06.015 为分析负压条件下柱形爆炸罐内爆炸波的传播特性,自行设计尺寸为320 mm× 430 mm的 可调真空度柱形爆炸罐,开展不同真空度条件下的内爆实验。通过内爆实验研究,获得了不同真空度下爆炸波的传播速度u、超压Δp、比冲量i、相对压力因子α和相对比冲量因子γ等爆炸波参数。结果表明:罐体内真空度的改变对爆炸波传播状态产生了显著影响,罐体内初始压力降低时,爆炸波超压和比冲量均有不同程度的衰减;当罐体内初始压力由常压降低至0.1 atm时,第1个爆炸波超压Δp<sub>1</sub>的相对压力因子α<sub>1max</sub>为2.41,第2个爆炸波超压Δp<sub>2</sub>的相对压力因子α<sub>2max</sub>为 1.64;第1个爆炸波比冲量i<sub>1</sub>的相对比冲量因子γ<sub>1max</sub>为6.97,第2个爆炸波比冲量i<sub>2</sub>的相对比冲量因子γ<sub>2max</sub>为3.14;α和γ分别反映了爆炸波超压和比冲量的衰减程度,α和γ的值越大表明爆炸波超压和比冲量衰减得越快;爆炸波的传播速度会随着初始环境压力的改变而发生变化,初始环境压力越低,爆炸波的传播速度越快。
WANG Q , LU J W , LI Z M , et al. Propagation law of explosion wave in columnar explosion tank under vacuum conditions [J ] . Acta Armamentarii , 2021 , 42 ( 6 ): 1250 - 1256 . (in Chinese) DOI: 10.3969/j.issn.1000-1093.2021.06.015 http://doi.org/10.3969/j.issn.1000-1093.2021.06.015 To analyze the propagation characteristics of explosion wave in a columnar explosion tank at negative pressure, the implosion test of a self-designed 320 mm×430 mm adjustable vacuum columnar explosion tank was made to obtain the blast wave propagation velocity u,overpressure Δp,specific impulse i, relative pressure factor α and relative specific impulse factor γ under different vacuum conditions. The results show that the change of vacuum in the tank has a significant effect on the propagation state of explosion wave,and when the initial pressure in the tank decreases,the explosion wave overpressure and specific impulse have different degrees of attenuation. When the initial pressure in the tank is reduced from atmospheric pressure to 0.1 atm, the relative pressure factor α<sub>1max</sub> of the first explosion wave Δp<sub>1</sub> is 2.41,and the relative pressure factor α<sub>2max</sub> of the second explosion wave Δp<sub>2</sub> is 1.64; the relative specific impulse factor γ<sub>1max</sub> of specific impulse i<sub>1</sub> of the first explosion wave is 6.97,and the relative specific impulse factor γ<sub>2max</sub> of specific impulse i<sub>2</sub> of the second explosion wave is 3.14. The relative pressure factor α and the relative specific impulse factor α reflect the degrees of attenuation of explosion wave overpressure and specific impulse,respectively,and the blast wave overpressure and specific impulse decay more quickly when α and γ are larger. In addition,the propagation speed of explosion wave changes with the change in the initial environmental pressure,and the lower the initial environmental pressure is,the faster the propagation speed of explosion wave is.
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