车辆堵塞下斜坡隧道火灾临界通风速度的数值研究

Huagang Liang, Liqin Pang, Dongmei Gao
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引用次数: 4

摘要

公路隧道位置的特殊性和空间的有限性导致其环境的封闭性,给疏散、救援、消防等活动增加了难度。本文利用火灾动力学模拟器进行数值模拟,研究了干扰对边坡隧道火灾临界速度的影响。本实验进行了两组工况模拟:(1)在直管巷道中,考虑放热率和堵塞比,并进行了数值模拟。(2)在20 MW火源放热速率下,考虑了隧道的堵塞比和坡度,并进行了数值模拟。车辆堵塞设置为火源上游两排两列分布,占隧道断面的6.6% ~ 22.0%。在0%、±1%、±2%、±3%、±4% 9种情况下选择坡度。6种放热速率分别为5 MW、10 MW、15 MW、20 MW、25 MW和30 MW。火灾发生在隧道中心线。结果表明:在平坦隧道中,临界流速随放热速率的变化趋势基本一致,且随放热速率的增大而增大;而在放热速率相同的情况下,车辆堵塞比越大,临界速度越小。从第二个实验案例可以看出,隧道坡度对临界速度的影响是不同的。在下坡隧道中,临界速度随坡度的增大而增大。在上坡隧道中,临界流速随坡度的增大而减小。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A numerical study on critical ventilation velocity in slope tunnel fire under vehicle blockage

The particularity of highway tunnel location and the limitation of space result in the closure of its environment, which makes evacuation, rescue, and firefighting activities more difficult. In this study, a fire dynamics simulator was used for numerical simulation to study the effect of jamming on the critical velocity of slope tunnel fire. This experiment carried out two sets of working conditions simulations: (1) In the straight tunnel, the heat release rate and the blockage ratio are considered and numerically simulated. (2) Under the heat release rate of 20 MW fire source, the blockage ratio and the gradient of the tunnel are considered and numerically simulated. The vehicle blockage is set to distribute in two rows and two columns upstream of the fire source, accounting for 6.6%-22.0% of the cross-section of the tunnel. The slopes were selected in nine cases of 0%, ±1%, ±2%, ±3%, and ±4%. The six heat release rates were 5 MW, 10 MW, 15 MW, 20 MW, 25 MW, and 30 MW, respectively. The fire occurred on the tunnel centerline. The results show that in flat tunnels, the variation trend of critical velocity with heat release rate is basically the same, and it increases with the increase of heat release rate. However, when the heat release rate is the same, the larger the vehicle blockage ratio is, the smaller the critical velocity is. It can be seen from the second experimental case that the influence of the tunnel slope on the critical velocity is different. In the downhill tunnel, the critical velocity increases with the increase of slope. In the uphill tunnel, the critical velocity decreases with the increase of slope.

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