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Inhibition of counterflow methane/air diffusion flame by water mist with varying mist diameter

机译:改变雾滴直径的水雾对逆流甲烷/空气扩散火焰的抑制

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摘要

In the present study, the effect of fine water mist on extinguishment of a methane-air counterflow diffusion flame was investigated to understand the underlying physics of fire extinguishment of highly stretched diffusion flame by water mist Twin-fluid atomizers were used to generate polydisperse water mist of which Sauter mean diameters were 10, 20, 40, and 60 μm. When water mist is not added, the critical stretch rate at extinguishment is 439 s~(-1) as compared to the theoretical value of 460 s~(-1) For the case with water mist addition, when the stretch rate is small enough, almost all the water mist evaporates within the flame zone. On the other hand, for high stretch rate case, large mist droplets pass through the flame zone and can reach the stagnation plane. However, no oscillatory motion was found around the stagnation plane. Critical stretch rate at extinguishment decreases monotonously with the mass fraction of water mist independently of the mist diameter within the range of D_(32) from 10 μm to 60 μm. On the other hand, with increase in the surface area parameter, the critical stretch rate at extinguishment decreases rapidly and becomes less sensitive at large surface area parameter, of which tendency is qualitatively in good agreement with theoretical predictions. For a constant surface area parameter, the critical stretch rate decreases with mist diameter because the mass fraction of water mist should increase in proportion to the mist diameter to keep the surface area parameter constant. When the water mist evaporates completely in the flame zone as in the present study, the mass fraction of the water mist is the dominant factor for fire extinguishment, rather than the surface area parameter. Therefore, an appropriate combination of stretch rate and water mist mass fraction should be provided to suppress effectively a given fire with a small amount of water mist.
机译:在本研究中,研究了细水雾对甲烷-空气逆流扩散火焰的灭火作用,以了解水雾对高拉伸扩散火焰进行灭火的基本原理。使用双流体雾化器生成多分散水雾其中Sauter的平均直径为10、20、40和60μm。当不添加水雾时,与460 s〜(-1)的理论值相比,灭火时的临界拉伸速率为439 s〜(-1)。对于添加水雾的情况,当拉伸速率足够小时,几乎所有的水雾都在火焰区内蒸发。另一方面,对于高拉伸率的情况,大的雾滴穿过火焰区并到达停滞平面。但是,在停滞平面周围未发现振荡运动。在D_(32)的范围从10μm到60μm的范围内,与水雾的质量分数无关地,灭火时的临界拉伸速率单调降低。另一方面,随着表面积参数的增加,熄灭时的临界拉伸速率迅速减小,并且在大表面积参数下变得不那么敏感,其趋势在质量上与理论预测吻合良好。对于恒定的表面积参数,临界拉伸速率随雾直径而降低,因为水雾的质量分数应与雾直径成比例增加,以保持表面积参数恒定。如本研究中所述,当水雾在火焰区中完全蒸发时,水雾的质量分数是灭火的主要因素,而不是表面积参数。因此,应提供拉伸速率和水雾质量分数的适当组合,以有效地抑制少量水雾给定的火灾。

著录项

  • 来源
    《Fire Safety Journal》 |2015年第1期|217-225|共9页
  • 作者单位

    Department of Mechanical Engineering, Tokyo Denki University, 5 Senju-Asahicho, Adachi-ku, Tokyo 120-8551, Japan;

    Department of Mechanical Engineering, Tokyo Denki University, 5 Senju-Asahicho, Adachi-ku, Tokyo 120-8551, Japan;

    Department of Mechanical Engineering, Tokyo Denki University, 5 Senju-Asahicho, Adachi-ku, Tokyo 120-8551, Japan;

    Fire Prevention Division, Fire and Disaster Management Agency, 2-1-2 Kasumigaseki, Chiyoda-ku, Tokyo 100-8927, Japan;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Fire suppression; Water mist; Extinguishment; Counterflow diffusion flame; Surface area parameter;

    机译:灭火;水雾灭火;逆流扩散火焰;表面积参数;

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