Flame Height of a Turbulent Diffusion Jet Flame with a Comparatively High Initial Discharging Velocity

Tomohiko Imamura, O. Sugawa, K. Kamiya, Y. Oka, Toshimitsu Suzuki, Yu-ichi Yamamoto
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引用次数: 3

Abstract

A series of experiments was carried out in order to investigate the visible flame height of a jet flame with a high initial discharging velocity where the fuel-release time and mass flow rate of fuel were varied. The values of non-dimensional heat release rate (Q*) in present experiment were in the range of 107 Q* 8. Even if the value of Q* was larger than 106, when the non-dimensional number (RM) employed by Heskestad which implies the ratio of gas release momentum to the momentum made by a purely buoyant diffusion flame was less than 0.1, the flame height with a comparatively high initial discharging velocity increased with the heat release rate. In other words, whether flame height depends on the Q*2/5 or not can be decided by the range of momentum ratio (RM) regardless of the range of non-dimensional heat release rate (Q*). This can be also decided by the fire Froude number employed by Delichatsios.
具有较高初始放电速度的湍流扩散射流火焰的火焰高度
为了研究高初速喷射火焰在不同燃料释放时间和燃料质量流量条件下的可见火焰高度,进行了一系列实验。无量纲放热率(Q*)在107 Q* 8范围内。即使Q*的值大于106,当Heskestad采用的非量纲数RM(即气体释放动量与纯浮力扩散火焰所产生的动量之比)小于0.1时,具有较高初始放电速度的火焰高度随着放热速率的增加而增加。换句话说,火焰高度是否取决于Q*2/5,可以由动量比(RM)的范围来决定,而不必考虑无因次放热率(Q*)的范围。这也可以由delihatsios使用的五个弗劳德数来决定。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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