共查询到19条相似文献,搜索用时 65 毫秒
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运用火灾动力学中的压力相似分析理论,推导出高海拔低压环境下的池火燃烧速率与常压环境下的相似关系,并结合前人实验数据,得到非受限燃烧条件下,等效直径在10~50 cm池火燃烧速率随气压降低呈线性变化的规律.通过开展拉萨低压地区及合肥常压地区的池火燃烧对比实验,并结合前人的实验数据对理论关系式进行验证,研究结果表明,压力相似分析虽仅从动力学角度出发,没有包含对燃烧化学机理的探讨,但仍然能够较好地反映出燃烧速率随环境压力的变化规律,对于指导实验研究,预测实验结果具有重要意义. 相似文献
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低气压环境下正庚烷及汽油池火的燃烧特性 总被引:1,自引:0,他引:1
为研究低气压环境对可燃物燃烧特性的影响,利用密闭实验箱模拟低气压环境条件,研究了正庚烷及汽油池火在不同环境压力条件下的燃烧特性.实验获取了燃料的质量燃烧速率、火焰形态特征、火焰温度和烟气中的CO体积分数等燃烧特性参数.研究结果表明,随着环境压力的降低,正庚烷和汽油的质量燃烧速率减小,且质量燃烧速率与环境压力呈幂函数关系;火焰高度及火焰面积均随环境压力的减小而增大,对于实验中的正庚烷池火,火焰高度与环境压力呈幂函数关系;环境压力的降低使得火焰的高温区上移,烟气羽流的温度也相应升高;烟气中CO的峰值体积分数也随着环境压力的降低而增大. 相似文献
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应用小尺寸火蔓延实验装置(FPA),在不同的外加辐射强度和燃烧环境氧体积分数条件下,对两种常见聚合物PMMA和POM的燃烧特性和传热阻碍的测量方法进行了实验研究.研究发现,两种燃料的无量纲燃烧质量损失速率与无量纲外加辐射热流之间存在确定的通用线性关系,即"燃烧质量损失速率基线";火焰传热阻碍系数分别高达0.4和0.3,它随燃烧环境氧体积分数增加而增大,但不随外加辐射强度变化.研究为发展火蔓延理论模型和燃料可燃性测试方法提供了重要的参考依据. 相似文献
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热塑性材料与底板间距对其燃烧行为的影响 总被引:2,自引:1,他引:1
为研究热塑性材料下端与底板间距对其熔融燃烧行为的影响,选择 6 mm厚和 4 mm厚 PP 板材作为研究对象,在 ISO 9705 燃烧室内进行了12组大尺寸燃烧实验,分别考虑了0cm、5 cm、10cm、15 cm、25 cm和35 cm不同间距的工况.实验过程中测量了热释放速率、消光系数、CO 体积分数以及温度场等火灾动力学参数.实验结果表明,热塑性材料的下边缘与底板的间距对火灾增长速率影响很大,但是对热释放速率峰值的影响不明显;随着间距的增加,壁面火和油池火之间的相互影响作用逐渐减弱,且当间距增加至 15 cm 以上时,各组实验的燃烧过程没有明显的区别. 相似文献
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根据通风条件不同,受限燃烧可分为燃料控制和通风控制两种燃烧状况。通风对于受限燃烧的火焰辐射有重要影响,尤其在通风控制燃烧时。本文以火焰中热量和炭颗粒的生成规律为基础,提出了描述通风影响的聚合物燃烧火焰辐射近似模型。针对几种典型聚合物计算了其火焰辐射放热分数和火焰平均辐射温度,并讨论了通风条件、燃烧构成和燃烧尺度的影响、以及火焰辐射放热分数与燃料烟点之间的关系。进而,在改进的基础上,以de Ris和 相似文献
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为了解风速对成品油库大型储罐池火灾事故发生后的池火火焰形态、热辐射分布以及对邻近储罐的影响,利用FLUENT软件,以全液面池火灾为基础,建立了有风工况和无风工况下50 000 m~3汽油储罐的事故模型。模拟发现:按照我国现行规范划定的储罐间间距,在发生单罐池火灾后,其邻近罐在任何风速工况下所接收到的热辐射值均在临界热辐射值13.5 kW/m~2之上;随着风速增大,强辐射区域逐渐由油池上方空间向油池下风方向空间蔓延,引起下风方向储罐二次事故的发生;事故罐邻近储罐,沿罐壁高度方向,热辐射值相差达22.1 kW/m~3,易造成储罐局部损坏。 相似文献
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A numerical study simulating the temporal vortical structures of a large-scale buoyant pool fire has been carried out using a fully-coupled Large Eddy Simulation (LES) model which incorporates all essential subgrid scale (SGS) turbulence, combustion, radiation and soot chemistry considerations. Based on the strained laminar flamelet approach, a scalar dissipation conditioned SGS combustion model is introduced to distinguish the highly non-equilibrating burn and extinguishment of flamelets commonly found in pool fires. Numerical results from the present model are validated and compared against a one-meter diameter methane pool fire experimental data and predictions from other LES field models. The predicted time-averaged velocity and temperature profiles have been found to be in good agreement with the experimental data and those numerical results. Qualitative comparisons of instantaneous velocity field against experimental data have revealed that the dynamic phenomena of large-scale vortical structures and its associated puffing behaviour of pool fire are well captured. Quantitative comparisons of velocity time history and pulsation frequency also show close agreement against experimentally evaluated quantities. 相似文献
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E. Studer D. Jamois S. Jallais G. Leroy J. Hebrard V. Blanchetière 《International Journal of Hydrogen Energy》2009
A future economy based on reduction of carbon-based fuels for power generation and transportation may consider hydrogen as possible energy carrier. Extensive and widespread use of hydrogen might require a pipeline network. The alternatives might be the use of the existing natural gas network or to design a dedicated network. Whatever the solution, mixing hydrogen with natural gas will modify the consequences of accidents, substantially. The French National Research Agency (ANR) funded project called HYDROMEL focuses on these critical questions. Within this project large-scale jet fires have been studied experimentally and numerically. The main characteristics of these flames including visible length, radiation fluxes and blowout have been assessed. 相似文献
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Miguel G. Cruz Bret W. Butler Domingos X. Viegas Pedro Palheiro 《Combustion and Flame》2011,(10):1970-1976
The present study is aimed at quantifying the flame radiosity vertical profile and gas temperature in moderate to high intensity spreading fires in shrubland fuels. We report on the results from 11 experimental fires conducted over a range of fire rate of spread and frontal fire intensity varying respectively between 0.04–0.35 m s−1 and 468–14,973 kW m−1. Flame radiosity, or radiant emissive power, and gas temperatures were measured with narrow angle radiometers and fine wire thermocouples located at three different heights in the flames, 0.6, 1.1 and 1.6 m above ground. Measured peak radiosity within the visual flame region (reaction zone and free flame) varied between 41 and 176 kW m−2. Measurements within the intermittent flame region above the visually estimated average flame height varied between 10 and 30 kW m−2. The flame vertical radiometric profile was characterized by a uniform area within the reaction zone and lower free flame, and a decrease in radiosity with height as the measurements approach the flame tip. 相似文献