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首页> 外文期刊>日本火災学会論文集 >横風中の火炎風下に発生する旋風に関する実験研究
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横風中の火炎風下に発生する旋風に関する実験研究

机译:逆风时火焰顺风产生旋风的实验研究

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摘要

大規模都市火災や森林火災では,旋風と呼ばれる竜 巻状の空気の渦が発生して大きな被害を引き起こすこ とがある.旋風は,その猛烈な風によって人や 物などを飛ばして被害をもたらすだけでなく,旋風 が火災域に近づけば,火炎を含んだ竜巻状の渦である 火災旋風に発展することもある.%Whirlwinds that occur downwind of a fire area were experimentally studied using flow visualization techniques and laser doppler velocimetry. Two types of experiments were performed. First, the effect of the complicated flow near the ground on the formation of whirlwinds downwind of a flame was investigated using an ethanol flame on a circular thin ceramic plate held in the middle of the test section of a wind tunnel using thin wires. It was demonstrated that the formation of whirlwinds downwind of the flame requires a floor beneath the flame. Secondly, the effects of cross-flow velocity and flame flickering on the characteristics of whirlwinds were investigated using the diffusion flame which was produced by injecting methane gas from a 30-mm diameter circular porous plate surface placed flush with the floor at a flow rate of 4.0 L/min into a cross-flow. The measured shedding frequency of the whirlwinds increased with increasing cross-flow velocity ranging from 0.13 to 0.37 m/s, corresponding to a Reynolds number from 262 to 727. The Strouhal number ranged from 0.05 to 0.42, which is much wider than the range of a Karman vortex wake in flow past a circular cylinder or of a jet wake in a cross-flow. The measured flame flickering frequency in the cross-flow ranged from 6.6 to 9.6 Hz and did not coincide with the whirlwind shedding frequency, which ranged from 0.3 to 4.2 Hz. The flickering frequency increased suddenly in a discontinuous manner at a cross-flow velocity of 0.28 m/s; this also did not coincide with the dependence of the whirlwind shedding frequency on the cross-flow velocity. The measured maximum tangential wind velocity of whirlwinds was almost constant at a cross-flow velocity ranging from 0.13 to 0.22 m/s.
机译:在大规模的城市大火和森林大火中,可能会发生称为旋风的龙卷风状空气涡流,并造成严重破坏。旋风不仅会由于强风而使人和物体飞扬而造成损坏,而且还可能发展成火焰旋风,当旋风接近着火区域时,旋风就像是含有火焰的龙卷风漩涡。使用流动可视化技术和激光多普勒测速仪,对着火区域顺风的%进行了实验研究,进行了两种类型的实验:首先,研究了地面附近复杂流动对火焰顺风形成的影响。使用乙醇火焰在一块圆形的薄陶瓷板上,用薄金属丝将其固定在风洞测试区域的中间,这证明了在火焰的顺风方向形成旋风需要在火焰下方有一层地板。使用扩散火焰研究了旋流特性上的横流速度和火焰闪烁,该扩散火焰是通过从直径为30毫米的圆形多孔板表面注入甲烷气体产生的,该多孔板与地面齐平,流速为4.0 L /分钟测得的旋风脱落频率随着横流速度从0.13到0.37 m / s的增加而增加雷诺数从262到727不等。斯特劳哈尔数的范围从0.05到0.42,远大于流经圆柱的卡曼涡旋尾流或横流的射流尾流的范围。横流中的火焰闪烁频率在6.6至9.6 Hz范围内,与旋风脱落频率在0.3至4.2 Hz的范围内不一致。在0.28 m的横流速度下,闪烁频率以不连续的方式突然增加/ s;这也与旋风脱落频率对横流速度的依赖性不一致。在0.13至0.22m / s的横流速度下,测得的旋风的最大切向风速几乎恒定。

著录项

  • 来源
    《日本火災学会論文集》 |2008年第1期|p.1-12|共12页
  • 作者

    篠原雅彦;

  • 作者单位

    消防研究センター(〒182-8500東 京都調布市深大寺東町4-35-3);

  • 收录信息
  • 原文格式 PDF
  • 正文语种 jpn
  • 中图分类 市政工程;
  • 关键词

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