当量比振荡在驱动低氮氧化物燃气轮机燃烧不稳定性中的作用

Tim Lieuwen, Ben T. Zinn
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引用次数: 396

摘要

本文对低氮氧化物燃气轮机在稀薄预混模式下的燃烧不稳定性进行了理论研究。结果表明,这些不稳定性可能是由燃烧室压力振荡与反应物供给速率的相互作用引起的,在进口管道中产生等效比扰动。这些扰动被平均气流对流到燃烧室,在那里它们产生大振幅的热释放振荡,驱动燃烧室压力振荡。本研究表明,与先前的分析相反,假设整个火焰区域的瞬时热释放均匀,火焰内的热释放可能表现出强烈的空间依赖性,这可以显著影响燃烧室的稳定性。提出的不稳定机制被纳入用于预测LNGT稳定极限的模型。模型结果表明,LNGT非常容易发生燃烧不稳定,特别是在精益工况下,不稳定区域可以用反应物从喷油器到燃烧器的对流时间和振荡周期的比值(对燃烧区域的结构进行一些修改)来近似描述。值得注意的是,开发的模型的预测与现有的实验数据非常吻合,有力地表明,提出的机制和开发的模型正确地解释了问题的基本物理性质。
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The role of equivalence ratio oscillations in driving combustion instabilities in low NOx gas turbines

This paper presents a theoretical investigation of combustion instabilities in low NOX gas turbines (LNGT) that burn fuel in a lean premixed mode. It is shown that these instabilities may be caused by interactions of combustor pressure oscillations with the reactants' supply rates, producing equivalence ratio perturbations in the inlet duct. These perturbations are convected by the mean flow to the combustor where they produce large-amplitude heat-release oscillations that drive combustor pressure oscillations. It is shown in this study that in contrast to earlier analyses, which assumed a uniform instantaneous heat release throughout the flame region, the heat release within the flame may exhibit strong spatial dependence that can significantly affect the combustor stability. The proposed instability mechanism is incorporated into a model that is used to predict LNGT stability limits. The model results show that LNGT are highly prone to combustion instabilities, especially under lean operating conditions, and that the regions of instability can be approximately described in terms of a ratio of the reactants' convective time from the fuel injector to the combustor and the period of the oscillations (with some modifications that account for the structure of the combustion region). Significantly, the developed model's predictions are in good agreement with available experimental data, strongly suggesting that the proposed mechanism and the developed model properly account for the essential physics of the problem.

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