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

机译:湍流火焰作为富氢燃料气体反吹倾向的指标

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The turbulent flame speed (S_T) 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 S_T/(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(S_T)被提出为燃气涡轮机相关条件下的富含氢气燃料气体的倒回倾销的指标。闪回是在将含有高氢含量的燃料气体引入燃气涡轮发动机时,闪回是不可避免的问题,其通常用天然气燃料。这些含氢燃料气体存在于综合气化联合循环(IGCC)的过程中,没有预燃烧碳捕获,以及具有各种惰性稀释度的合成气(H_2 + CO)和氢气中的含量。因此需要对这些混合物的闪回现象的更多了解,以便将IGCC概念(无碳捕获)进化为清洁发电的有希望的候选者。与合成气相比,富含氢气混合物的富含氢气混合物在稀薄吹出和闪回的发生之间表现出较窄的操作包络。当发生闪回时,发现火焰传播仅在管道的边界层中供应预混燃料/空气混合物到燃烧器。该发现基于湍流,瘦预混,无旋流,限制射流的实验研究,用于三种燃料混合物的H_2> 70 Vol。 %。在燃烧器入口处(U_0 = 40m / s)处的固定散装速度下测量最多10个条形,并且预热温度(T_0 = 623 k)。通过OH-PLIF诊断检索火焰前部特性,并且通过全局消耗率的角度,通过湍流速度(S_T)得到了湍流火焰速度(S_T)。关于闪回限制,发现富含氢混合物的操作范围由燃料(G_c)和流量(G_F)分别规定的速度梯度优质。前者(G_C)被确定为S_T /(LE×Δ_(L0)),其中LE是lewis号,Δ_(l0)是计算的一维层状火焰的热厚度。后者(G_F)被Blasius相关性预测完全发育的湍流管流,并且它表示流动可以抵消相反的火焰传播的能力。我们的结果表明,两个速度梯度达到相似水平的等效比对应于在各种压力下观察到的倒回限制。还发现该方法能够预测合成气与富含氢混合物之间的操作范围的上述差异。

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