在不同先导级当量比下运行的中央分级燃烧器中的火焰宏观结构和热声不稳定性

Jingyuan Xiang, Jiacheng Li, Weishu Mo, Bo Wang, Dong Yang, Xiaohua Gan
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摘要

本文的重点是发现中央分段漩涡燃烧器中火焰宏观结构与热声不稳定性之间的联系。在实际的燃烧器中,先导级的流量远小于主级的流量。然而,在保持类似总流量的情况下,先导阶段的改动可能会改变火焰的宏观结构。因此,在相同的主级入口条件下,通过改变先导级的等效比,对不同火焰宏观结构下的热声不稳定性进行了研究。通过高频平面激光测量和化学发光测量,提高了空间和时间精度,从而更全面地了解了热声不稳定性。根据预热区的分布,确定了两种不同的火焰宏观结构,即 S 型和 I 型火焰。它们表现出不同的热声不稳定性,其中 I 型火焰比 S 型火焰表现出更强烈的不稳定性。结果表明,火焰宏观结构的变化会影响火焰热释放与流场的耦合。具体来说,I 型火焰的预热区和热释放对流场波动的敏感性更高,从而导致火焰的波动更强烈、更复杂。这种差异导致了热声不稳定性强度的变化,以及热释放和声压之间相位耦合的变化,进而影响了总瑞利指数。同时,I 型和 S 型火焰在流场波动的分布模式和范围上也存在显著差异。
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The flame macrostructure and thermoacoustic instability in a centrally staged burner operating in different pilot stage equivalence ratios
The main focus of this paper is to discover the link between flame macrostructure and thermoacoustic instability in a centrally staged swirl burner. In practical combustors, the flow rate in the pilot stage is much smaller than that in the main stage. However, the modification in the pilot stage could alter the flame macrostructure while maintaining a similar total flow rate. Therefore, the thermoacoustic instability was examined at different flame macrostructures by varying the pilot stage equivalence ratio under identical main stage inlet conditions. High-frequency planar laser measurements and chemiluminescence measurement were conducted to enhance spatial and temporal accuracy, providing a more comprehensive understanding of thermoacoustic instability. Two different flame macrostructures, S-type and I-type flames, were identified based on the preheating zone distribution. They exhibit distinct thermoacoustic instabilities, with the I-type flames demonstrating more intense instability than S-type flames. The results indicate that the variation of flame macrostructure influences the coupling of flame heat release and flow field. Specifically, the preheating zone and heat release of I-type flames exhibit greater sensitivity to flow field fluctuations, resulting in a more intense and complex fluctuation of the flame. This discrepancy leads to variations in thermoacoustic instability intensity, as well as the changes in the phase coupling between heat release and acoustic pressure, which in turn impact the total Rayleigh index. Meanwhile, significant differences exist in the distribution pattern and range of flow field fluctuations between I-type and S-type flames.
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