柱状药包不同位置起爆爆生气体演化规律

Evolution patterns of detonation gas under different initiation positions in cylindrical charges

  • 摘要: 合理提高爆炸能量利用率是岩石爆破的重要研究课题,爆生气体在钻孔爆破中起着重要作用,但是针对柱状药包爆生气体演化机理的研究还有待深入。为探究爆生气体的演化规律,通过纹影试验系统进行了柱状药包的爆炸试验,分析了不同位置起爆条件下柱状药包爆生气体演化规律。结果表明:柱状药包爆生气体的演化过程分为膨胀、流动和自由扩散3个阶段。气体分布特征由爆轰波数量和传播方向决定,顶点起爆时爆生气体流场即单个爆轰波形成的气体流场,中点起爆和1/3点起爆时则2个相反运动的爆轰波形成的气体流场叠加形成,叠加后的流场分布特征取决于叠加前的流场动量,这是起爆位置影响爆生气体分布特征的根本原因。爆生气体产生后会向起爆位置流动,产生聚集效应。顶点起爆时,在空气反压的作用下气体堆积在起爆位置形成聚集区域;中点起爆时,两股相同动量的气流在起爆位置汇聚,轴向动量抵消形成聚集区;1/3点起爆时,两股动量不同的气流在起爆位置汇聚形成聚集区,高动量的部分气流会穿过聚集区继续沿轴向流动。聚集效应由强到弱依次为中点起爆> 1/3点起爆>顶点起爆,气体在径向的最大流动距离同样如此。爆生气体的聚集效应促进了聚集区气体的径向流动,使得起爆位置气体的径向流动距离远大于其他位置。

     

    Abstract: Improving the utilization efficiency of explosive energy is a crucial research topic in rock blasting. Detonation gas plays a significant role in borehole blasting, yet there is limited research on the evolution patterns of detonation gas from cylindrical charges. Utilizing an explosion schlieren experimental system, experiments on cylindrical charges were conducted to analyze the evolution patterns of detonation gas under different initiation positions. The results show that the evolution process of the detonation gas from the cylindrical charge can be divided into three stages: expansion, flow, and free diffusion. The distribution characteristics of detonation gas from cylindrical charges are determined by the number and propagation direction of detonation waves. When the initiation occurs at the apex, the gas flow field is formed by a single detonation wave. In contrast, initiation at the midpoint or one-third of the charge length results in a gas flow field formed by the superposition of two oppositely moving detonation waves. The distribution characteristics of the superimposed flow field depend on the momentum of the flow fields before superposition, which fundamentally explains how initiation position influences the distribution characteristics of detonation gas. The detonation gases flow towards the initiation point, resulting in a convergence effect. With apex initiation, gas converges at the initiation position due to the counter pressure of air, forming an convergence region. With midpoint initiation, two gas flows of equal momentum converge at the initiation position, their axial momenta canceling out to form an convergence region. With one-third point initiation, two gas flows of different momenta converge at the initiation position, forming an convergence region, with the higher momentum flow continuing to move axially through the convergence region. The convergence effect order based on initiation position is: midpoint initiation > one-third point initiation > apex initiation, with the maximum radial flow distance of the gas following the same order. This convergence effect of detonation gas promotes radial gas flow in the convergence region, resulting in the radial flow distance at the initiation position being much greater than at other positions.

     

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