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TURBULENT FLAME SPEED AS AN INDICATOR FOR FLASHBACK PROPENSITY OF HYDROGEN-RICH FUEL GASES

机译:湍流火焰速度作为富含氢气燃料气体汽油倾向的指示灯

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The turbulent flame speed (ST) is proposed to be an indicator of flashback propensity for hydrogen-rich fuel gases at gas turbine relevant conditions. Flashback is an inevitable issue to be concerned about when introducing fuel gases containing high hydrogen content to gas turbine engines, which are conventionally fueled with natural gas. These hydrogen-containing fuel gases are present in the process of the integrated gasification combined cycle (IGCC) with and without pre-combustion carbon capture, and both syngas (H_2 + CO) and hydrogen with various degree of inert dilution fall in this category. More understanding on the flashback phenomenon for these mixtures is thus necessary in order to evolve the IGCC concept (either with or without carbon capture) into a promising candidate for clean power generation. Compared to syngas, the hydrogen-rich fuel mixtures exhibit an even narrower operational envelope between the occurrence of lean blow out and flashback. When flashback occurs, the flame propagation is found to happen exclusively in the boundary layer of the pipe supplying the premixed fuel/air mixture to the combustor. This finding is based on the experimental investigation of turbulent, lean-premixed, non-swirled, confined jet flames for three fuel mixtures with H_2 > 70 Vol.%. Measurements were performed up to 10 bar at fixed bulk velocity at the combustor inlet (u_0 = 40 m/s) and preheat temperature (T_0 = 623 K). Flame front characteristics were retrieved via OH-PLIF diagnostics, and turbulent flame speed (S_T) was derived accordingly from the perspective of a global consumption rate. Concerning the flashback limit, the operational range of the hydrogen-rich mixtures is found to be well represented by the velocity gradients prescribed respectively by the flame (g_c) and the flow (g_f). The former (g_c) is determined as ST/(Le × δ_(L0)), where Le is the Lewis number and δ_(L0) is the calculated thermal thickness of the one-dimensional laminar flame. The latter (g_f) is predicted by the Blasius correlation for fully developed turbulent pipe flow, and it indicates the capability with which the flow can counteract the opposed flame propagation. Our results show that the equivalence ratios at which the two velocity gradients reach similar levels correspond well to the flashback limits observed at various pressures. The methodology is also found to be capable of predicting the aforementioned difference in the operational range between syngas and hydrogen-rich mixtures.
机译:湍流火焰速度(ST)建议成为回火倾向的在燃气涡轮机相关条件富氢燃料气体的指示符。闪回要关注引入含有氢含量高到燃气涡轮发动机,其通常用天然气作燃料的燃料气体时的不可避免的问题。这些含氢燃料气体存在于集成气化联合循环(IGCC)的具有和不具有预燃烧碳捕集过程中,和这两个合成气(H_2 + CO)和氢气与该类别中不同程度的惰性稀释落下。对这些混合物的逆燃现象更加理解因此,有必要的,以便演化的IGCC概念(具有或不具有碳捕获)到用于清洁发电有希望的候选。相比合成气,所述富含氢气的燃料混合物表现出贫油熄火和回火的发生之间的甚至更窄的操作包络线。当回火发生时,火焰传播被发现在管供给预混合的燃料/空气混合物在燃烧器的边界层只发生。这一发现是基于湍流的实验研究,稀薄预混合的,非涡旋,密闭喷射火焰为三个燃料混合物与H_2> 70体积%。测量在在燃烧器入口(U_0 = 40米/秒)的固定本体速度和预热温度(T_0 = 623 K)执行到10巴。火焰前缘特性经由OH-PLIF诊断检索,并且是从全球消耗率的角度相应地衍生湍流火焰速度(S_T)。关于回火限制,富氢的混合物的操作范围被发现是由分别由火焰(g_c)规定的速度梯度和流(g_f)得到很好的体现。前者(g_c)被确定为ST /(LE×δ_(L0)),其中乐是路易斯数和δ_(L0)是一维层流火焰的计算出的热的厚度。后者(g_f)由用于充分发展的湍流管流的布拉休斯相关预测,并且它指示与该流动可以抵消相对火焰传播的能力。我们的结果表明,当量比在该两个速度梯度达到相似水平对应很好地在各种压力下所观察到的逆燃极限。该方法也被发现能够预测合成气和富氢气体的混合物之间的操作范围前述差的。

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