Nonlinear dynamics and thermoacoustic intermittency of a hydrogen-powered sequential combustor

IF 6.2 2区 工程技术 Q2 ENERGY & FUELS Combustion and Flame Pub Date : 2025-02-09 DOI:10.1016/j.combustflame.2025.114008
Matteo Impagnatiello, Sergey Shcherbanev, Bayu Dharmaputra, Nicolas Noiray
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By increasing the thermal power of the first stage, thermoacoustic instabilities arise in both configurations, albeit with distinct behaviors. <span><math><msub><mrow><mi>F</mi></mrow><mrow><msub><mrow><mi>CH</mi></mrow><mrow><mn>4</mn></mrow></msub></mrow></msub></math></span> exhibits a gradual onset of instability, whereas <span><math><msub><mrow><mi>F</mi></mrow><mrow><msub><mrow><mi>H</mi></mrow><mrow><mn>2</mn></mrow></msub></mrow></msub></math></span> undergoes a subcritical Hopf bifurcation, characterized by abrupt, intermittent transitions between a linearly stable state and limit cycles at intermediate first-stage power. Distinct acoustic pressure spectra are observed during instability: <span><math><msub><mrow><mi>F</mi></mrow><mrow><msub><mrow><mi>CH</mi></mrow><mrow><mn>4</mn></mrow></msub></mrow></msub></math></span> features a single dominant peak around 290 Hz, while <span><math><msub><mrow><mi>F</mi></mrow><mrow><msub><mrow><mi>H</mi></mrow><mrow><mn>2</mn></mrow></msub></mrow></msub></math></span> displays multiple high-amplitude peaks corresponding to harmonics of the fundamental frequency near 400 Hz. Analysis of acoustic pressure and OH* chemiluminescence during instability reveals a strong coupling between acoustic fluctuations and autoignition kernel formation. With <span><math><msub><mrow><mi>F</mi></mrow><mrow><msub><mrow><mi>CH</mi></mrow><mrow><mn>4</mn></mrow></msub></mrow></msub></math></span>, the temporal evolution of the OH* chemiluminescence associated with these kernels follows a quasi-sinusoidal profile at the instability frequency, whereas with <span><math><msub><mrow><mi>F</mi></mrow><mrow><msub><mrow><mi>H</mi></mrow><mrow><mn>2</mn></mrow></msub></mrow></msub></math></span>, it consists of sharp pulses synchronized with the fundamental acoustic mode. Although existing Low-Order Models (LOMs) successfully capture the experimental behavior in <span><math><msub><mrow><mi>F</mi></mrow><mrow><msub><mrow><mi>CH</mi></mrow><mrow><mn>4</mn></mrow></msub></mrow></msub></math></span>, they fail to replicate the complex dynamics of <span><math><msub><mrow><mi>F</mi></mrow><mrow><msub><mrow><mi>H</mi></mrow><mrow><mn>2</mn></mrow></msub></mrow></msub></math></span>. To address this, a novel LOM incorporating a strongly nonlinear Heat Release Rate (HRR) feedback term is developed, specifically tailored for configurations with significant coupling between autoignition and thermoacoustics. This model successfully replicates the key spectral features of <span><math><msub><mrow><mi>F</mi></mrow><mrow><msub><mrow><mi>H</mi></mrow><mrow><mn>2</mn></mrow></msub></mrow></msub></math></span>, underscoring the need for advanced models to accurately reproduce the complex thermoacoustic behavior of sequential combustors. The findings of this study provide a deeper understanding of the challenges associated with sequential combustors operating under autoignition conditions, particularly in the context of decarbonization through 100% hydrogen operation.</div><div><strong>Novelty and Significance Statement</strong></div><div>This study presents, for the first time, experimental results from a lab-scale constant-pressure sequential combustor fired with pure hydrogen in both stages. The behavior under pure hydrogen fueling is compared with that of a methane–hydrogen blend. In both cases, a strong coupling is observed between autoignition kernel formation and thermoacoustic instabilities. However, the acoustic pressure spectra under pure hydrogen fueling exhibit distinct and atypical features compared to those obtained with the methane–hydrogen blend. The critical role of autoignition kernels in triggering and sustaining these instabilities is highlighted. Additionally, a novel Low-Order Model is proposed, accurately replicating the key spectral features observed in the pure hydrogen case. These findings provide valuable insights for the community, supporting the transition to pure hydrogen fueling in sequential combustors under autoigniting conditions.</div></div>","PeriodicalId":280,"journal":{"name":"Combustion and Flame","volume":"274 ","pages":"Article 114008"},"PeriodicalIF":6.2000,"publicationDate":"2025-02-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Combustion and Flame","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S001021802500046X","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENERGY & FUELS","Score":null,"Total":0}
引用次数: 0

Abstract

This study experimentally investigates the coupling between thermoacoustic instabilities and autoignition kernel formation in Constant Pressure Sequential Combustors (CPSCs). Two fuel types are examined: a less reactive methane–hydrogen blend (FCH4) and pure hydrogen (FH2). By increasing the thermal power of the first stage, thermoacoustic instabilities arise in both configurations, albeit with distinct behaviors. FCH4 exhibits a gradual onset of instability, whereas FH2 undergoes a subcritical Hopf bifurcation, characterized by abrupt, intermittent transitions between a linearly stable state and limit cycles at intermediate first-stage power. Distinct acoustic pressure spectra are observed during instability: FCH4 features a single dominant peak around 290 Hz, while FH2 displays multiple high-amplitude peaks corresponding to harmonics of the fundamental frequency near 400 Hz. Analysis of acoustic pressure and OH* chemiluminescence during instability reveals a strong coupling between acoustic fluctuations and autoignition kernel formation. With FCH4, the temporal evolution of the OH* chemiluminescence associated with these kernels follows a quasi-sinusoidal profile at the instability frequency, whereas with FH2, it consists of sharp pulses synchronized with the fundamental acoustic mode. Although existing Low-Order Models (LOMs) successfully capture the experimental behavior in FCH4, they fail to replicate the complex dynamics of FH2. To address this, a novel LOM incorporating a strongly nonlinear Heat Release Rate (HRR) feedback term is developed, specifically tailored for configurations with significant coupling between autoignition and thermoacoustics. This model successfully replicates the key spectral features of FH2, underscoring the need for advanced models to accurately reproduce the complex thermoacoustic behavior of sequential combustors. The findings of this study provide a deeper understanding of the challenges associated with sequential combustors operating under autoignition conditions, particularly in the context of decarbonization through 100% hydrogen operation.
Novelty and Significance Statement
This study presents, for the first time, experimental results from a lab-scale constant-pressure sequential combustor fired with pure hydrogen in both stages. The behavior under pure hydrogen fueling is compared with that of a methane–hydrogen blend. In both cases, a strong coupling is observed between autoignition kernel formation and thermoacoustic instabilities. However, the acoustic pressure spectra under pure hydrogen fueling exhibit distinct and atypical features compared to those obtained with the methane–hydrogen blend. The critical role of autoignition kernels in triggering and sustaining these instabilities is highlighted. Additionally, a novel Low-Order Model is proposed, accurately replicating the key spectral features observed in the pure hydrogen case. These findings provide valuable insights for the community, supporting the transition to pure hydrogen fueling in sequential combustors under autoigniting conditions.
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氢动力序贯燃烧器的非线性动力学和热声间歇性
实验研究了恒压序贯燃烧室热声不稳定性与自燃核形成之间的耦合关系。测试了两种燃料类型:反应性较低的甲烷氢混合物(FCH4)和纯氢(FH2)。通过增加第一级的热功率,两种结构都出现了热声不稳定性,尽管具有不同的行为。FCH4表现出逐渐开始的不稳定性,而FH2则经历亚临界Hopf分岔,其特征是在线性稳定状态和极限环之间的突然间歇过渡。在不稳定过程中观察到不同的声压谱:FCH4在290 Hz左右具有单个主导峰,而FH2在400 Hz附近显示多个高振幅峰,对应于基频谐波。对不稳定过程中声压和OH*化学发光的分析揭示了声波动和自燃核形成之间的强耦合。在FCH4中,与这些核相关的OH*化学发光在不稳定频率下的时间演化遵循准正弦曲线,而在FH2中,它由与基本声学模式同步的尖锐脉冲组成。尽管现有的低阶模型(LOMs)成功地捕获了FCH4的实验行为,但它们无法复制FH2的复杂动力学。为了解决这个问题,开发了一种新型LOM,其中包含强烈非线性热释放率(HRR)反馈项,专门针对自燃和热声学之间存在显著耦合的配置进行了定制。该模型成功地复制了FH2的关键光谱特征,强调了对先进模型的需求,以准确地再现顺序燃烧室的复杂热声行为。这项研究的结果让我们更深入地了解了在自燃条件下运行的顺序燃烧器所面临的挑战,特别是在通过100%氢气运行脱碳的情况下。新颖性和意义声明:本研究首次提出了在两个阶段使用纯氢的实验室规模恒压顺序燃烧器的实验结果。比较了纯氢加氢和甲烷-氢混合燃料的性能。在这两种情况下,观察到自燃核形成和热声不稳定性之间的强耦合。然而,与甲烷-氢混合燃料相比,纯氢燃料下的声压谱表现出明显的非典型特征。强调了自燃核在触发和维持这些不稳定性中的关键作用。此外,提出了一个新的低阶模型,准确地复制了在纯氢情况下观测到的关键光谱特征。这些发现为社区提供了有价值的见解,支持在自燃条件下顺序燃烧器向纯氢燃料的过渡。
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来源期刊
Combustion and Flame
Combustion and Flame 工程技术-工程:化工
CiteScore
9.50
自引率
20.50%
发文量
631
审稿时长
3.8 months
期刊介绍: The mission of the journal is to publish high quality work from experimental, theoretical, and computational investigations on the fundamentals of combustion phenomena and closely allied matters. While submissions in all pertinent areas are welcomed, past and recent focus of the journal has been on: Development and validation of reaction kinetics, reduction of reaction mechanisms and modeling of combustion systems, including: Conventional, alternative and surrogate fuels; Pollutants; Particulate and aerosol formation and abatement; Heterogeneous processes. Experimental, theoretical, and computational studies of laminar and turbulent combustion phenomena, including: Premixed and non-premixed flames; Ignition and extinction phenomena; Flame propagation; Flame structure; Instabilities and swirl; Flame spread; Multi-phase reactants. Advances in diagnostic and computational methods in combustion, including: Measurement and simulation of scalar and vector properties; Novel techniques; State-of-the art applications. Fundamental investigations of combustion technologies and systems, including: Internal combustion engines; Gas turbines; Small- and large-scale stationary combustion and power generation; Catalytic combustion; Combustion synthesis; Combustion under extreme conditions; New concepts.
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