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Radiative extinction of gaseous spherical diffusion flames in microgravity

机译:微重力下气态球形扩散火焰的辐射消光

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Radiative extinction of spherical diffusion flames was investigated experimentally and numerically. The experiments involved microgravity spherical diffusion flames burning ethylene and propane at 0.98 bar. Both normal (fuel flowing into oxidizer) and inverse (oxidizer flowing into fuel) flames were studied, with nitrogen supplied to either the fuel or the oxygen. Flame conditions were chosen to ensure that the flames extinguished within the 2.2 s of available test time; thus extinction occurred during unsteady flame conditions. Diagnostics included color video and thin-filament pyrometry. The computations, which simulated flow from a porous sphere into a quiescent environment, included detailed chemistry, transport, and radiation and yielded transient results. Radiative extinction was observed experimentally and simulated numerically. Extinction time, peak temperature, and radiative loss fraction were found to be independent of flow rate except at very low flow rates. Radiative heat loss was dominated by the combustion products downstream of the flame and was found to scale with flame surface area, not volume. For large transient flames the heat release rate also scaled with surface area and thus the radiative loss fraction was largely independent of flow rate. Peak temperatures at extinction onset were about 1100 K, which is significantly lower than for kinetic extinction. An important observation of this work is that while radiative heat losses can drive transient extinction, this is not only because radiative losses are increasing with time but also because the heat release rate is falling off as the flame expands away from the burner and the reactant supply to the flame decreases.
机译:对球形扩散火焰的辐射消光进行了实验和数值研究。实验涉及在0.98巴下燃烧乙烯和丙烷的微重力球形扩散火焰。研究了正常火焰(流入氧化剂的燃料)和反火焰(氧化剂流入燃料)的火焰,并向燃料或氧气供应了氮气。选择火焰条件以确保火焰在可用测试时间的2.​​2 s内熄灭;因此,在不稳定的火焰条件下会熄灭。诊断包括彩色视频和细丝高温测定。该计算模拟了从多孔球体到静态环境的流动,包括详细的化学,传输和辐射,并产生了瞬态结果。实验观察了辐射消光并进行了数值模拟。发现消光时间,峰值温度和辐射损耗分数与流速无关,除非流速非常低。辐射热损失主要由火焰下游的燃烧产物决定,并随火焰表面积而不是体积成比例增加。对于大的瞬态火焰,放热率也随表面积成比例变化,因此辐射损失分数在很大程度上与流速无关。灭绝开始时的峰值温度约为1100 K,大大低于动力学灭绝时的峰值温度。这项工作的一个重要观察结果是,尽管辐射热损失会导致瞬态熄灭,这不仅是因为辐射损失随时间增加,而且还因为火焰从燃烧器和反应物供应移开,放热率下降了。火焰减少。

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