体积分数差和多孔介质对甲烷爆炸双向传播的影响实验研究

    Experimental study on effects of volume fraction difference and porous media on bidirectional propagation of methane explosion

    • 摘要: 为研究瓦斯爆炸双向传播规律和受抑制效果,在自主搭建的爆炸管道平台上进行了实验研究。水平管道系统由3段各1 m长的透明有机玻璃管组成,实验中各段管道充入不同体积分数的甲烷/空气混合气,中间偏右点火,爆炸火焰向两侧传播;左右管道中各放置1片多孔介质,观测不同孔隙密度介质对爆炸传播的影响,并对爆炸过程的火焰图像、传播速度和爆炸超压进行分析。结果表明:孔隙密度10 ppi(1 ppi=39.37孔/m)的多孔介质对火焰产生激励效果(加速火焰传播),孔隙密度20 ppi和30 ppi的多孔介质对火焰产生抑制效果;点火位置在中间偏右,火焰会先到达右边多孔介质,此时右边比左边的多孔介质对火焰传播的激励或抑制效果更明显;在甲烷体积分数差和多孔介质共同作用下,从中心向左和向右传播的火焰速度曲线呈“组合W”形,即向左和向右传播火焰前锋速度都出现了缓慢增长阶段、向下波动阶段和快速上升阶段,左边多孔介质孔隙密度变化对爆炸火焰向右传播的影响很小(在右边多孔介质孔隙密度相同时,火焰传播到管道右端的时间相同),而右边多孔介质孔隙密度变化对爆炸火焰向左传播的影响较大(当右边多孔介质变化,则火焰传播到管道左端的时间差异较大);左边孔隙密度30 ppi、右边孔隙密度10 ppi的多孔介质工况中,向左传播火焰越过多孔介质一段距离后仍然会熄灭;左右组合多孔介质方式都能有效降低爆炸超压,左边孔隙密度30 ppi、右边孔隙密度20 ppi的多孔介质工况下的爆炸传播速度最慢、爆炸超压最小。

       

      Abstract: To investigate the bidirectional propagation law and inhibition effect of gas explosions, experimental studies were conducted on a self-built explosion pipeline platform. The horizontal pipeline system was composed of three transparent acrylic glass sections each with a length of 1 m. In the experiments, each section was filled with methane/air mixtures of different volume fractions, ignition was initiated at a position slightly to the right of the center, and the explosion flame propagated to both sides. One piece of porous medium was placed in each of the left and right pipelines to observe the influence of porous media with different pore densities on explosion propagation. The flame images, propagation velocity and explosion overpressure during the explosion process were all analyzed. The results show that porous medium with a pore density of 10 ppi (1 ppi=39.37 pores per meter) exerts an excitation effect on the flame (accelerates its propagation), while porous media with pore densities of 20 ppi and 30 ppi produce an inhibition effect on the flame. With ignition at the position slightly to the right of the center, the flame reaches the porous medium on the right first, and the excitation or inhibition effect of the right porous medium on flame propagation is more significant than that of the left one at this time. Under the combined action of methane volume fraction difference and porous media, the flame velocity curves for propagation from the center to the left and right present a combined W-shape, meaning the velocities of the flame fronts propagating leftward and rightward all undergo a slow growth stage, a downward fluctuation stage and a rapid rise stage. The variation in pore density of the left porous medium has a negligible effect on the rightward propagation of the explosion flame (with the same pore density of the right porous medium, the time for the flame to propagate to the right end of the pipeline is consistent). In contrast, the variation in pore density of the right porous medium exerts a considerable influence on the leftward propagation of the explosion flame (the time for the flame to reach the left end of the pipeline varies significantly with the change of the right porous medium). In the working condition of porous medium with pore density of 30 ppi on the left and 10 ppi on the right, the flame propagating leftward still extinguishes after traveling a certain distance past the porous medium. The combined arrangement of porous media on both the left and right sides can effectively reduce the explosion overpressure. The explosion propagation velocity is the slowest and the explosion overpressure is the minimum under the working condition with porous medium with pore density of 30 ppi on the left and 20 ppi on the right.

       

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