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A phenomenological understanding of the multimodal low-frequency oscillating combustion of ammonia induced by filamentary plasma discharge 从现象学角度理解丝状等离子体放电诱导氨的多模式低频振荡燃烧
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-26 DOI: 10.1016/j.combustflame.2024.113748
This work finds that with the assistance of filamentary plasma discharge, the ammonia combustion becomes very complicated with multiple modes, especially including a low-frequency (<2 Hz) oscillating combustion mode. This flame oscillation, which is sensitive to the discharge characteristics and the flow/fuel/boundary conditions, can be further categorized as three sub-modes denoted as Mode C1, C2 and C3. Their transitions occur depending on the flow rate (Qtot), the equivalence ratio (ϕ) and the temperature of the chamber wall. Detailed dynamic characteristics of flame kernels and flow fields during the oscillating process are further acquired to confirm the changing recirculation zone and the Karlovitz (Ka) number. A phenomenological mechanism based on recirculated energy feedback is thus proposed to explain the oscillating flame. In addition, the S-curve is used to elucidate the plasma impacts on the complicated combustion characteristics, especially the oscillating combustion modes and their transitions. It is found that the folded S-curve can be stretched with the help of plasma discharge. By considering the energy feedback effects, the S-curve can become more stretched with the Da number for extinction (i.e. DaE) being larger than that for ignition (i.e. DaI). Meanwhile, the branch with the Da number between DaI and DaE is unstable and the multiple oscillating combustion modes (i.e. Mode C1-C3) can be categorized on the unstable branch of the stretched S-curve.
这项研究发现,在丝状等离子体放电的帮助下,氨燃烧变得非常复杂,具有多种模式,特别是包括低频(2 赫兹)振荡燃烧模式。这种火焰振荡对放电特性和流量/燃料/边界条件非常敏感,可进一步分为三种子模式,分别称为模式 C1、C2 和 C3。它们的转换取决于流量(Qtot)、等效比(j)和腔壁温度。在振荡过程中,进一步获取了火焰内核和流场的详细动态特性,以确认不断变化的再循环区和卡尔洛维茨(Ka)数。因此,提出了一种基于再循环能量反馈的现象学机制来解释振荡火焰。此外,S 曲线还用于阐明等离子体对复杂燃烧特性的影响,特别是振荡燃烧模式及其转换。研究发现,在等离子体放电的帮助下,折叠的 S 曲线可以被拉伸。考虑到能量反馈效应,S 曲线的拉伸程度越大,熄灭的 Da 值(即 DaE′)就越大于点火的 Da 值(即 DaI′)。同时,Da 数介于 DaI′ 和 DaE′ 之间的分支是不稳定的,多重振荡燃烧模式(即模式 C1-C3)可归类于拉伸 S 曲线的不稳定分支上。
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引用次数: 0
The effect of hydrogen enrichment on the conical premixed methane–air flame response and thermoacoustic modes coupling 氢气富集对锥形预混合甲烷-空气火焰响应和热声模式耦合的影响
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-24 DOI: 10.1016/j.combustflame.2024.113742
This paper investigates the thermoacoustic dynamic responses of hydrogen-enriched laminar premixed conical methane–air flames under dual-mode coupling. Utilizing the level set method and the G-equation model, one meticulously derives the flame describing function (FDF) in relation to variations in hydrogen enrichment levels (ηH). This precisely derived FDF is then integrated into the low-order network model of the Rijke tube to analyze the thermoacoustic unstable modes of the system. Finally, dual-frequencies incoming flow velocity perturbations are reintroduced as inputs to obtain the flame response under thermoacoustic modes coupling. Results show that while keeping the unstretched steady flame aspect ratio constant, an increase in ηH not only raises the FDF’s cut-off frequency but also enhances the FDF gain within the nonlinear frequency region, leading to more unstable modes, especially high frequency modes within the Rijke tube system. Furthermore, the flame response is further altered under the excitation of dual unstable modes. When both modes are within the linear frequency region of the FDF, the flame response is co-controlled by the two modes, predominantly by the mode with a larger velocity perturbation amplitude, with weaker modes coupling leading to the additional frequency perturbation having a suppressive effect on the flame response at the original frequency. Conversely, when one or two modes are within the nonlinear frequency region of the FDF, the flame response is dominated by the lower-frequency mode, with higher nonlinear modes coupling allowing the additional frequency perturbation to both promote and suppress the response at the original frequency and also couple to produce a significant difference frequency response. Novelty and significance The novelty of this paper lies in the determination of the flame describing function (FDF) with varying hydrogen enrichment levels and the stability of thermoacoustic systems, and more significantly, conducting an in-depth and comprehensive investigation into the nonlinear dynamic responses of hydrogen-enriched flames to different types of dual-mode coupling perturbations. The dual-mode perturbations result in either attenuation or amplification of the flame response, depending on whether the corresponding frequencies lie within the linear or nonlinear frequency regions of the FDF, which innovatively incorporates the influence of the FDF phase and examines the responses at the difference frequencies generated by the coupling. This lays a foundation for further exploration into the mechanisms of modes coupling in hydrogen-enriched and other thermoacoustic systems.
本文研究了双模式耦合下富氢层流预混合锥形甲烷-空气火焰的热声动态响应。利用水平集方法和 G-方程模型,我们细致地推导出了与氢富集水平(ηH)变化相关的火焰描述函数(FDF)。然后将精确推导出的 FDF 与 Rijke 管的低阶网络模型相结合,分析系统的热声不稳定模式。最后,重新引入双频流入流速扰动作为输入,以获得热声模式耦合下的火焰响应。结果表明,在保持未拉伸稳定火焰长宽比不变的情况下,ηH 的增加不仅会提高 FDF 的截止频率,还会增强非线性频率区域内的 FDF 增益,从而导致更多的不稳定模式,尤其是里克管系统内的高频模式。此外,在双重不稳定模式的激励下,火焰响应会发生进一步变化。当两个模式都在 FDF 的线性频率区域内时,火焰响应由两个模式共同控制,主要由速度扰动幅度较大的模式控制,较弱的模式耦合导致额外的频率扰动对原始频率的火焰响应产生抑制作用。相反,当一个或两个模态处于 FDF 的非线性频率区域内时,火焰响应主要由频率较低的模态主导,较高的非线性模态耦合使得附加频率扰动既能促进又能抑制原始频率的响应,还能耦合产生显著的差频响应。新颖性和意义 本文的新颖性在于确定了不同富氢水平下的火焰描述函数(FDF)以及热声系统的稳定性,更重要的是对富氢火焰对不同类型双模耦合扰动的非线性动态响应进行了深入而全面的研究。双模扰动会导致火焰响应的衰减或放大,这取决于相应频率是位于 FDF 的线性频率区还是非线性频率区,该研究创新性地纳入了 FDF 相位的影响,并考察了耦合产生的差频响应。这为进一步探索富氢和其他热声系统中的模式耦合机制奠定了基础。
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引用次数: 0
Investigation of Al-Li particle ignition dynamics with different Li content 不同锂含量下的铝锂粒子点火动力学研究
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-24 DOI: 10.1016/j.combustflame.2024.113734
Promoting the ignition of aluminum powder is considered an effective method to inhibit the agglomeration of aluminum powder in propellants and enhance combustion efficiency. This study utilizes laser ignition technology and high-speed photography to investigate the ignition and combustion processes of single aluminum particles and aluminum-lithium alloy particles. The focus is on comparing the effects of the diameter of micron-sized metal particles and the lithium content in aluminum-lithium alloy particles on the ignition and combustion processes of metal particles. The results show that the ignition delay time is directly proportional to the diameter of the metal particles and inversely proportional to the lithium content. For the aluminum-lithium alloy particle with a lithium content of 3.5 %, even if the diameter is close to 300 μm, the ignition delay time is only 125.5 ms, which is much smaller than that of the pure aluminum particle with a diameter of 208 μm. Compared to aluminum particles and aluminum-lithium alloy particles, there is basically no difference between the two during the combustion stage. However, in the ignition stage, aluminum-lithium alloy particles sequentially exhibit a red gas-phase flame corresponding to lithium and a yellow gas-phase flame corresponding to aluminum. This indicates that during the ignition process of aluminum-lithium alloy particles, lithium first reacts with the oxidative atmosphere and releases heat, providing a heat source for the subsequent ignition of aluminum particles. This also explains why the ignition delay time of metal particles is inversely proportional to the lithium content. An ignition model for aluminum particles in a multi-component atmosphere is established, which further considers the chemical reactions between lithium and oxidative gases, making the model applicable to aluminum-lithium alloy particles. This ignition model effectively describes the impact of particle diameter and lithium content on the ignition process of metal particles. The model is further verified, and the results show that the calculated ignition delay is in good agreement with the experimental data. Overall, this study provides deeper experimental and theoretical insights into the ignition and combustion processes of aluminum-lithium alloys, and the findings can guide the application of aluminum-lithium alloys in propellants.
促进铝粉点火被认为是抑制推进剂中铝粉结块和提高燃烧效率的有效方法。本研究利用激光点火技术和高速摄影技术研究了单个铝颗粒和铝锂合金颗粒的点火和燃烧过程。重点比较了微米级金属颗粒直径和铝锂合金颗粒中锂含量对金属颗粒点火和燃烧过程的影响。结果表明,点火延迟时间与金属颗粒直径成正比,与锂含量成反比。对于锂含量为 3.5 % 的铝锂合金颗粒,即使直径接近 300 μm,点火延迟时间也只有 125.5 ms,远小于直径为 208 μm 的纯铝颗粒。铝粒子和铝锂合金粒子相比,在燃烧阶段两者基本没有差别。然而,在点火阶段,铝锂合金颗粒依次呈现出与锂相对应的红色气相火焰和与铝相对应的黄色气相火焰。这表明,在铝锂合金颗粒的点火过程中,锂首先与氧化气氛发生反应并释放热量,为随后铝颗粒的点火提供热源。这也解释了为什么金属颗粒的点火延迟时间与锂含量成反比。该模型进一步考虑了锂与氧化性气体之间的化学反应,使其适用于铝锂合金颗粒。该点火模型有效地描述了颗粒直径和锂含量对金属颗粒点火过程的影响。对模型进行了进一步验证,结果表明计算出的点火延迟与实验数据十分吻合。总之,本研究为铝锂合金的点火和燃烧过程提供了更深入的实验和理论见解,研究结果可指导铝锂合金在推进剂中的应用。
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引用次数: 0
Effect of gravity and pressure on soot formation in laminar inverse diffusion flames at elevated pressures 重力和压力对高压下层流反向扩散火焰中烟尘形成的影响
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-24 DOI: 10.1016/j.combustflame.2024.113747
Inverse diffusion flame (IDF) configuration, where the oxidizer is surrounded by fuel, is commonly used in reforming of hydrocarbon fuels for hydrogen production through the autothermal reforming and partial oxidation processes. Understanding the mechanism of soot formation in IDF is crucial for achieving efficient and environmentally friendly hydrogen production. In this study, high-fidelity numerical simulations were conducted to investigate the effects of pressure and gravity on the soot formation in a laminar IDF configuration at pressures up to 20 bar. The chemical kinetic models with detailed polycyclic aromatic hydrocarbons (PAH) pathways and an empirical reactive soot inception model are employed. The simulation results agreed well with experimental measurements, showing consistency in flame height, PAH concentration, and soot volume fraction. The simulations accurately reproduced the spatial distributions of PAHs and soot in the IDF, and quantitatively captured the linear increase in peak soot volume fraction with pressure. The linear relationship is mainly attributed to the linear increase in the PAH concentration, driven by changes in density due to pressure increase. Moreover, compared to zero gravity condition, higher flame temperature and radical concentrations were observed in normal gravity, leading to higher soot formation rates. However, buoyancy accelerates fluid movement, reducing residence time and ultimately suppressing soot formation in normal gravity conditions.
反向扩散火焰(IDF)配置是指氧化剂被燃料包围,通常用于碳氢化合物燃料的重整,通过自热重整和部分氧化过程制氢。了解 IDF 中烟尘的形成机理对于实现高效、环保的氢气生产至关重要。本研究进行了高保真数值模拟,以研究压力和重力对压力高达 20 巴的层流 IDF 配置中烟尘形成的影响。采用了包含详细多环芳烃(PAH)路径的化学动力学模型和经验反应烟尘萌发模型。模拟结果与实验测量结果一致,显示出火焰高度、多环芳烃浓度和烟尘体积分数的一致性。模拟结果准确地再现了多环芳烃和烟尘在 IDF 中的空间分布,并定量地捕捉到了烟尘体积分数峰值随压力的线性增加。这种线性关系主要归因于多环芳烃浓度的线性增加,而这种增加是由压力增加引起的密度变化驱动的。此外,与零重力条件相比,正常重力条件下的火焰温度和自由基浓度更高,从而导致更高的烟尘形成率。然而,浮力加速了流体运动,缩短了停留时间,最终抑制了正常重力条件下的烟尘形成。
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引用次数: 0
Ignition envelope and bubbly spray combustion of a cost-effective self-igniting fuel with rocket-grade hydrogen peroxide 使用火箭级过氧化氢的经济高效自燃燃料的点火包络和气泡喷雾燃烧
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-24 DOI: 10.1016/j.combustflame.2024.113744
Since the beginning of this century, the space industry has been searching for stable non-toxic propellants to replace hydrazine-based fuels. In this paper, we introduce a novel eco-friendly self-igniting fuel, denoted PAHyp 3, which comprises a blend of N,N,N′,N′-tetramethylethylenediamine (TMEDA) and N-methylethanolamine (MMEA) catalyzed with a copper-based catalyst. This promising formulation is coupled with hydrogen peroxide as the oxidizer. To map near-optimal formulations in terms of performance and chemical stability, we varied the proportions of MMEA and TMEDA, each catalyzed with copper nitrate trihydrate concentrations ranging from 0.25% to 3% by weight. Drop tests revealed that a 50:50 mixture of TMEDA and MMEA, catalyzed with 2 wt% copper nitrate trihydrate, exhibited a rapid ignition delay time (IDT) of approximately 14 ms when paired with 94% hydrogen peroxide. This composition was subsequently chosen for evaluation using an impinging jet apparatus capable of capturing simultaneous visible and shadowgraph high-speed imaging, facilitating the detailed study of the ignition process. Screenshots from impinging jet firing tests unveiled that the majority of ignition events, utilizing 94% hydrogen peroxide, occurred downstream less than 20 ms after impingement. Subsequently, foam-like structures engulfed the vaporized and combusted liquid sheet, emitting stable orange/green flames. These promising outcomes indicate that PAHyp 3 presents novel prospects in aerospace propulsion, with the potential to replace hazardous and toxic hydrazine-based propellants. Moreover, a model was proposed to explain how bubble nucleation and growth from hydrogen peroxide decomposition can enhance atomization, leading to a new atomization mode we have termed “catalytic decomposition-assisted atomization”.
自本世纪初以来,航天工业一直在寻找稳定无毒的推进剂来替代肼基燃料。本文介绍了一种新型环保自燃燃料 PAHyp 3,它由 N,N,N′,N′-四甲基乙二胺(TMEDA)和 N-甲基乙醇胺(MMEA)在铜基催化剂催化下混合而成。这种前景广阔的配方与作为氧化剂的过氧化氢配合使用。为了绘制出在性能和化学稳定性方面接近最佳的配方,我们改变了 MMEA 和 TMEDA 的比例,每种配方在三水硝酸铜催化下的浓度从 0.25% 到 3% (按重量计)不等。跌落测试表明,在 2 wt% 的三水硝酸铜催化下,50:50 的 TMEDA 和 MMEA 混合物与 94% 的过氧化氢配对时,可显示出约 14 毫秒的快速点火延迟时间 (IDT)。随后,我们选择了这种成分,使用可同时捕捉可见光和阴影图高速成像的撞击喷射装置进行评估,从而促进了对点火过程的详细研究。冲击射流点火试验的截图显示,使用 94% 过氧化氢的大多数点火事件都发生在冲击后不到 20 毫秒的下游。随后,泡沫状结构吞噬了汽化和燃烧的液态薄片,发出稳定的橙色/绿色火焰。这些令人鼓舞的结果表明,PAHyp 3 在航空航天推进方面具有新的前景,有可能取代危险和有毒的肼基推进剂。此外,我们还提出了一个模型,用于解释过氧化氢分解产生的气泡成核和增长如何增强雾化效果,从而产生了一种新的雾化模式,我们称之为 "催化分解辅助雾化"。
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引用次数: 0
An experimental investigation on a flow-facilitated ignition at reduced and normal pressures for small, near-unity and large Lewis number of hydrogen/air and hydrogen/ammonia/air mixtures 关于氢气/空气和氢气/氨气/空气混合物在减压和常压下流动促进点火的实验研究,涉及氢气/空气和氢气/氨气/空气混合物的小路易斯数、近统一路易斯数和大路易斯数
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-23 DOI: 10.1016/j.combustflame.2024.113746
At sufficiently small spark gap (dgap=0.64 mm) and at sub-atmospheric pressure (p = 0.3 atm), a numerical simulation by Chen et al. (2023) reported a flow-facilitated ignition (FFI) phenomenon in an imposed uniform flow perpendicular to a pair of electrodes, where a constant ignition energy (Eig=1.24 mJ) cannot ignite the hydrogen/air mixture at an equivalence ratio ϕ=0.4 with small Lewis number Le≈0.43<<1 in quiescence but ignition is successful in flowing conditions. This implied that the occurrence of FFI was mainly due to heat losses regardless of Le in contradiction with previous turbulence-facilitated ignition results. To test FFI, a well-controlled ignition experiment at dgap=0.6 mm using the same simulation flow-electrode concept via a uniform flow setup resided in a large pressure-controlled chamber with optical access is conducted for three targeted mixtures having Le≈0.43<<1 (H2/air at ϕ=0.4), Le≈2.3>>1 (H2/air at ϕ=5.1), and Le≈0.95∼1 ((80%NH3+20%H2)/air at ϕ=1). Various Eig=0.2∼250 mJ of high accuracy are applied to measure minimum ignition energies (MIE) at 50% ignitability under static and flowing conditions with an inlet flow velocity (Uin=0–10 m/s) at p = 0.3 atm and/or 1 atm. Experimental results show no FFI for Le≈0.43<<1 and Le≈0.95∼1 cases even at p = 0.3 atm, because values of MIE increase gradually with increasing Uin. However, FFI does occur for Le≈2.3>>1 case, since Eig=250 mJ cannot ignite static mixture at p = 1 atm and MIE decreases drastically from 151.8 mJ at Uin=1 m/s to 30.1 mJ at Uin=4 m/s. These results provide important information of the effects of uniform flow on electrode-spark (forced) ignition of premixed flames, revealing two key points: (i) Heat losses alone cannot lead to FFI, because FFI does not occur at Le∼1 and Le<<1 cases even at p = 0.3 atm. (ii) FFI only occurs at sufficiently large Le>>1 and sufficiently small dgap.
在足够小的火花间隙(dgap=0.64 mm)和亚大气压(p = 0.3 atm)条件下,Chen 等人(2023 年)的数值模拟报告了在垂直于一对电极的强加均匀流中的流动促进点火(FFI)现象。24 mJ)无法点燃等效比 ϕ=0.4 且路易斯数 Le≈0.43<<1 较小的静态氢气/空气混合物,但在流动条件下点火成功。这意味着发生 FFI 的主要原因是热损失,而与 Le 无关,这与之前的湍流促进点火结果相矛盾。为了测试 FFI,在 dgap=0.6 mm 的条件下,使用相同的模拟流-电极概念,通过一个位于大型压力控制室中的均匀流装置,对三种目标混合物进行了良好的点火实验,这些混合物的 Le≈0.43<<1(H2/空气,j=0.4)、Le≈2.3>>1(H2/空气,j=5.1)和 Le≈0.95∼1((80%NH3+20%H2)/空气,j=1)。在 p = 0.3 atm 和/或 1 atm 的静态和流动条件下,以入口流速(Uin=0-10 m/s)测量 50%可燃性时的最小点火能量(MIE),各种 Eig=0.2∼250 mJ 的精度都很高。实验结果表明,即使在 p = 0.3 atm 的条件下,Le≈0.43<<1 和 Le≈0.95∼1 的情况下也不会出现 FFI,因为 MIE 值会随着 Uin 的增加而逐渐增大。然而,Le≈2.3>>1 情况下确实发生了 FFI,因为 Eig=250 mJ 无法在 p=1 atm 时点燃静态混合物,MIE 从 Uin=1 m/s 时的 151.8 mJ 急剧下降到 Uin=4 m/s 时的 30.1 mJ。这些结果提供了均匀流动对预混合火焰电火花(强制)点火影响的重要信息,揭示了两个关键点:(i) 仅热损失不会导致 FFI,因为即使在 p = 0.3 atm 时,FFI 也不会在 Le∼1 和 Le<<1 情况下发生。(ii) 只有在 Le>>1 足够大和 dgap 足够小的情况下,才会出现 FFI。
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引用次数: 0
The role of low/high- temperature chemistry in computationally reproducing flame stabilization modes of hydrogen-fueled supersonic combustion 低温/高温化学在计算再现氢燃料超音速燃烧火焰稳定模式中的作用
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-21 DOI: 10.1016/j.combustflame.2024.113711

Numerical simulations of two typical flame stabilization modes in a cavity-assisted supersonic combustor were performed using improved delay detached eddy simulation and three hydrogen oxidation mechanisms with different levels of fidelity. The simulation results with Burke's detailed mechanism agree well with the experimental measurements in terms of flame morphology and wall pressure, in both jet-wake and cavity flame modes. The comparative study shows that, lacking necessary intermediate species, Eklund's reduced mechanism and Marinov's global mechanism incorrectly yield jet wake stabilization mode under low inflow stagnation temperature T0. Through computational singular perturbation analysis, a sequential radical triggering mechanism was identified for flame stabilization, wherein the reaction R1: H+O2=O+OH dominates in fuel jet wake forming OH and O radicals, the reaction R2: H2+O=H+OH controls the reaction between H2 and O forming the OH radical pool, and then the heat release completes via R3: H2+OH=H+H2O. However, their activation differs in the two stabilization modes. The role of transport is key in the cavity flame mode, where the colder stream inhibits auto-ignition in the jet wake, activating low-temperature chemistry, and delaying R2 in the cavity region. Thus, the presence of H2O2 and HO2 species was found to be essential for accurately reproducing the flame stabilization in the cavity flame stabilization mode, whereas their effect is marginal in jet wake mode. In fact, the jet-wake flame stabilization is characterized by auto-ignition under high inflow stagnation temperatures, with the chain-branching reaction R2 activating in the fuel jet-wake, causing an explosive dynamic therein. These findings suggest the H2O2 and HO2 species and associated low-temperature reactions are necessary for the accurate prediction of the flame stabilization mode under low T0, whereas their absence does not affect the prediction of the flame mode under high T0, in which case all three chemical mechanisms give reasonably good agreements in flame characteristics and engine overall performances.

利用改进的延迟分离涡模拟和三种不同逼真度的氢氧化机制,对空腔辅助超音速燃烧器中的两种典型火焰稳定模式进行了数值模拟。采用伯克详细机制的模拟结果与实验测量结果在火焰形态和壁压方面非常吻合,无论是在喷射醒焰模式还是空腔火焰模式。比较研究表明,由于缺乏必要的中间物种,埃克伦德的简化机制和马林诺夫的全局机制在低流入停滞温度 T0 下错误地产生了喷气唤醒稳定模式。通过计算奇异扰动分析,确定了火焰稳定的顺序自由基触发机制,其中反应 R1:H+O2=O+OH 在燃料喷射尾流中起主导作用,形成 OH 和 O 自由基;反应 R2:H2+O=H+OH 在燃料喷射尾流中起主导作用,形成 OH 和 O 自由基:H2+O=H+OH 控制 H2 和 O 之间的反应,形成 OH 自由基池,然后通过 R3:H2+OH=H+H2O 完成热量释放。然而,在两种稳定模式中,它们的活化作用是不同的。在空腔火焰模式中,传输的作用非常关键,较冷的气流会抑制喷射尾流中的自燃,激活低温化学反应,并延迟空腔区域中的 R2。因此,在空腔火焰稳定模式中,H2O2 和 HO2 物种的存在对于准确再现火焰稳定至关重要,而在喷气唤醒模式中,它们的作用微乎其微。事实上,喷射-唤醒火焰稳定的特点是在高流入停滞温度下自燃,燃料喷射-唤醒中的链式支化反应 R2 被激活,在其中引起爆炸动态。这些发现表明,要准确预测低 T0 下的火焰稳定模式,H2O2 和 HO2 物种及相关的低温反应是必要的,而缺少它们并不影响对高 T0 下火焰模式的预测,在这种情况下,所有三种化学机制在火焰特性和发动机整体性能方面都有相当好的一致性。
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引用次数: 0
Multiple-point ignition as a driver of flame acceleration at the early stage of burning in channels 多点着火是通道燃烧初期火焰加速的驱动因素
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-21 DOI: 10.1016/j.combustflame.2024.113743

In the present study, flame acceleration driven by an array of multiple ignition kernels, equally spaced in the axial direction of a channel closed at one end, is studied numerically. In order to demonstrate the effects of the proposed ignition configuration on the flow dynamics, free-slip wall boundary condition is adopted. It is demonstrated that the burning of multiple flame kernels generates a powerful upstream flow, propelling the flame kernels, with the leading kernel’s tip undergoing a strong exponential acceleration. In a channel with smooth walls, such a powerful acceleration process is limited in time. The present study is mainly focused on the dynamics of the flame during the exponential stage of acceleration. The dependence of the acceleration rate, total acceleration time, and the maximum flame velocity on the initial distance between the kernels, the number of ignition kernels, and the thermal gas expansion coefficient, is quantified. Remarkably, the initial distance between the kernels has a weak influence on the above mentioned characteristics of flame dynamics as long as it is sufficiently large. It is observed that the acceleration rate increases with the kernel number. Notably, a significantly large maximum flame tip velocity can be achieved using the multi-kernel configuration as compared to the single-point ignition scenario. The acceleration rate demonstrates a nearly linear dependence on the thermal expansion coefficient, thus, the increase in thermal expansion results in a considerably stronger flame acceleration process.

Novelty and Significance Statement

For the first time, the flame acceleration process upon simultaneous ignition of a multi-point array of hot kernels equally spaced at the centerline of a channel was systematically studied. The work emphasizes the potential for achieving an extremely high flame speed within a very short time as compared to the single-ignition method. The acceleration rate, total acceleration time, and maximum achievable flame velocity were quantified. In a multi-point ignition scenario, we demonstrate that the burning of the fresh mixture between the kernels increases an overall cumulative gas expansion, propelling the leading tip. This result suggests a method for creating a powerful flame acceleration, which is an essential step in deflagration-to-detonation transition. Notably, the powerful acceleration is achieved in channels with smooth walls, which is important for DDT applications, in which using obstructed channels may be associated with a range of operational problems. The simplicity of the setup is also emphasized.

本研究以数值方法研究了在一端封闭的通道轴向等间距排列的多个点火核驱动的火焰加速。为了证明所提出的点火配置对流动动力学的影响,采用了自由滑壁边界条件。结果表明,多个焰核的燃烧会产生强大的上游气流,推动焰核的燃烧,其中前导焰核的顶端会受到强烈的指数加速。在壁面光滑的通道中,这种强大的加速过程在时间上是有限的。本研究主要关注火焰在指数加速阶段的动态。研究量化了加速率、总加速时间和最大火焰速度与点火芯之间的初始距离、点火芯数量和热气体膨胀系数的关系。值得注意的是,只要内核间的初始距离足够大,它对上述火焰动力学特征的影响就很微弱。据观察,加速度随核数的增加而增加。值得注意的是,与单点点火方案相比,使用多核配置可以获得明显更大的最大焰尖速度。加速率与热膨胀系数几乎呈线性关系,因此,热膨胀系数的增加会导致火焰加速过程大大加强。 新颖性和意义声明首次系统地研究了在通道中心线等间距多点热核阵列同时点火时的火焰加速过程。与单点点火法相比,该研究强调了在极短的时间内实现极高火焰速度的潜力。对加速率、总加速时间和可达到的最大火焰速度进行了量化。在多点点火的情况下,我们证明了果核间新鲜混合物的燃烧增加了整体累积气体膨胀,推动了前端。这一结果表明了一种产生强大火焰加速度的方法,而火焰加速度是爆燃到爆燃转变过程中必不可少的一步。值得注意的是,这种强大的加速度是在壁面光滑的通道中实现的,这对滴滴涕应用非常重要,因为在这种应用中,使用有障碍的通道可能会带来一系列操作问题。该装置的简易性也得到了强调。
{"title":"Multiple-point ignition as a driver of flame acceleration at the early stage of burning in channels","authors":"","doi":"10.1016/j.combustflame.2024.113743","DOIUrl":"10.1016/j.combustflame.2024.113743","url":null,"abstract":"<div><p>In the present study, flame acceleration driven by an array of multiple ignition kernels, equally spaced in the axial direction of a channel closed at one end, is studied numerically. In order to demonstrate the effects of the proposed ignition configuration on the flow dynamics, free-slip wall boundary condition is adopted. It is demonstrated that the burning of multiple flame kernels generates a powerful upstream flow, propelling the flame kernels, with the leading kernel’s tip undergoing a strong exponential acceleration. In a channel with smooth walls, such a powerful acceleration process is limited in time. The present study is mainly focused on the dynamics of the flame during the exponential stage of acceleration. The dependence of the acceleration rate, total acceleration time, and the maximum flame velocity on the initial distance between the kernels, the number of ignition kernels, and the thermal gas expansion coefficient, is quantified. Remarkably, the initial distance between the kernels has a weak influence on the above mentioned characteristics of flame dynamics as long as it is sufficiently large. It is observed that the acceleration rate increases with the kernel number. Notably, a significantly large maximum flame tip velocity can be achieved using the multi-kernel configuration as compared to the single-point ignition scenario. The acceleration rate demonstrates a nearly linear dependence on the thermal expansion coefficient, thus, the increase in thermal expansion results in a considerably stronger flame acceleration process.</p><p><strong>Novelty and Significance Statement</strong></p><p>For the first time, the flame acceleration process upon simultaneous ignition of a multi-point array of hot kernels equally spaced at the centerline of a channel was systematically studied. The work emphasizes the potential for achieving an extremely high flame speed within a very short time as compared to the single-ignition method. The acceleration rate, total acceleration time, and maximum achievable flame velocity were quantified. In a multi-point ignition scenario, we demonstrate that the burning of the fresh mixture between the kernels increases an overall cumulative gas expansion, propelling the leading tip. This result suggests a method for creating a powerful flame acceleration, which is an essential step in deflagration-to-detonation transition. Notably, the powerful acceleration is achieved in channels with smooth walls, which is important for DDT applications, in which using obstructed channels may be associated with a range of operational problems. The simplicity of the setup is also emphasized.</p></div>","PeriodicalId":280,"journal":{"name":"Combustion and Flame","volume":null,"pages":null},"PeriodicalIF":5.8,"publicationDate":"2024-09-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142271972","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
A theoretical and kinetic study of key reactions between ammonia and fuel molecules, part III: H-atom abstraction from esters by ṄH2 radicals 氨与燃料分子间关键反应的理论和动力学研究,第三部分:ṄH2 自由基从酯中抽取 H 原子
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-21 DOI: 10.1016/j.combustflame.2024.113738

Hydrogen atom abstraction reactions by ṄH2 radicals play a crucial role in determining the reactivity of ammonia/fuel binary blends. Esters are a typical component of environmentally friendly and economically promising biofuels. The feasibility of the ammonia/biofuel dual-fuel approach has been proven in practical engines. [Energy and Fuels 22 (2008) 2963] and [Int. J. Energy Res. 2023 (2023) 9920670]. ṄH2 radicals play a critical role in the combustion and pyrolysis chemistry of ammonia and N-containing-rich fuels. In ammonia/biofuels hybrid combustion, ṄH2 radicals can react with biofuel molecules in a reaction class that is particularly important especially when sufficient ammonia is blended in order to eliminate NOx emissions. To help unravel the chemistry of ammonia/biofuel blends, a systematic theoretical kinetic study of H-atom abstraction from eleven alky esters of CnH2n+1COOCH3 (n = 1–4), CH3COOCmH2m+1 (m = 1–4), and C2H5COOC2H5, by ṄH2 radicals is performed in this work. The geometry optimization, frequency, and zero-point energy calculations for all related species, as well as the hindrance potential energy surface for low frequency torsional modes in the reactants and transition states, were performed at the M06–2X/6–311++G(d,p) level of theory. Intrinsic reaction coordinate calculations were performed to validate the connections between the transition states and expected minima energy species. The energies of all of the species involved were calculated at the QCISD(T)/cc-pVXZ (X = D, T, Q) and MP2/cc-pVYZ (Y = T, Q) levels of theory and then extrapolated to the complete basis set. Rate constants of 39 reactions were calculated using the Master Equation System Solver (MESS) program in the temperature range of 500 – 2000 K. These rate constants for different H-atom abstraction sites are provided and can be extrapolated to larger esters. The kinetic effects from the functional group are also illustrated by performing detailed comparisons with the previous studies of ṄH2 radical reactions with alkanes, alcohols and ethers.

ṄH2自由基的氢原子抽取反应在决定氨/燃料二元混合物的反应性方面起着至关重要的作用。酯类是环保且具有经济前景的生物燃料的典型成分。氨/生物燃料双燃料方法的可行性已在实际发动机中得到证实。[能源与燃料 22 (2008) 2963]和[能源研究国际期刊 2023 (2023) 9920670]。ṄH2自由基在氨和富含氮的燃料的燃烧和热解化学过程中起着至关重要的作用。在氨/生物燃料混合燃烧中,ṄH2 自由基可与生物燃料分子发生反应,这种反应尤其重要,特别是当为了消除氮氧化物排放而掺入足够的氨时。为了帮助揭示氨/生物燃料混合物的化学性质,本研究对ṄH2 自由基从 CnH2n+1COOCH3 (n = 1-4)、CH3COOCmH2m+1 (m = 1-4)和 C2H5COOC2H5 的十一种烷基酯中抽取 H 原子进行了系统的理论动力学研究。在 M06-2X/6-311++G(d,p) 理论水平上对所有相关物种进行了几何优化、频率和零点能计算,并计算了反应物和过渡态中低频扭转模的阻碍势能面。为了验证过渡态与预期最小能量物种之间的联系,还进行了本征反应坐标计算。在 QCISD(T)/cc-pVXZ (X = D, T, Q) 和 MP2/cc-pVYZ (Y = T, Q) 理论水平上计算了所有涉及物种的能量,然后外推到完整的基集。在 500 - 2000 K 的温度范围内,使用主方程系统求解器 (MESS) 程序计算了 39 个反应的速率常数。通过与以前研究的ṄH2 自由基与烷烃、醇和醚的反应进行详细比较,还说明了官能团对动力学的影响。
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引用次数: 0
Symbolic construction of the chemical Jacobian of quasi-steady state (QSS) chemistries for Exascale computing platforms 面向超大规模计算平台的准稳态(QSS)化学雅各布函数的符号构建
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-09-20 DOI: 10.1016/j.combustflame.2024.113740

The Quasi-Steady State Approximation (QSSA) can be an effective tool for reducing the size and stiffness of chemical mechanisms for implementation in computational reacting flow solvers. However, for many applications, the resulting model still requires implicit methods for efficient time integration. In this paper, we outline an approach to formulating the QSSA reduction that is coupled with a strategy to generate C++ source code to evaluate the net species production rates, and the chemical Jacobian. The code-generation component employs a symbolic approach enabling a simple and effective strategy to analytically compute the chemical Jacobian. For computational tractability, the symbolic approach needs to be paired with common subexpression elimination which can negatively affect memory usage. Several solutions are outlined and successfully tested on a 3D multipulse ignition problem, thus allowing portable application across chemical model sizes and GPU capabilities. The implementation of the proposed method is available at https://github.com/AMReX-Combustion/PelePhysics under an open-source license.

Novelty and Significance

A symbolic method is proposed to write analytical chemical Jacobians. The benefit of the symbolic method is that it is easy to implement and flexible to any elementary reaction type. Its benefit is shown in the context of QSS-reduced chemistries: there, constructing an analytical chemical Jacobian is complex since one must include the effect of traditional elementary reactions and algebraic closure for the QSS species. To the authors’ knowledge, there is no open-source package available to construct analytical Jacobians of QSS-reduced chemistries. We expect this work to facilitate the use of analytical Jacobians in arbitrarily complex chemical mechanisms. The proposed method was integrated into an open-source suite of reacting flow solvers https://github.com/AMReX-Combustion/PelePhysics to facilitate its dissemination.

准稳态近似法(QSSA)是在计算反应流求解器中减少化学机制的大小和刚度的有效工具。然而,在许多应用中,生成的模型仍然需要隐式方法进行有效的时间积分。在本文中,我们概述了一种制定 QSSA 简化的方法,该方法与一种生成 C++ 源代码的策略相结合,可用于评估物种净生产率和化学雅各布。代码生成部分采用了一种符号方法,能够以简单有效的策略分析计算化学雅各比。为了提高计算的可操作性,符号方法需要与常用子表达式消除法搭配使用,这可能会对内存使用产生负面影响。本文概述了几种解决方案,并成功地在三维多脉冲点火问题上进行了测试,从而实现了化学模型大小和 GPU 性能的可移植应用。该方法的实现可在 https://github.com/AMReX-Combustion/PelePhysics 上以开源许可的方式获得。新颖性和意义提出了一种符号方法来编写分析化学雅各比。这种符号方法的优点是易于实现,而且对任何基本反应类型都很灵活。这种方法的优点在 QSS 还原化学中得到了体现:在 QSS 还原化学中,构建解析化学雅各布因子非常复杂,因为必须包括传统基本反应的影响和 QSS 物种的代数闭合。据作者所知,目前还没有可用的开源软件包来构建 QSS 还原化学的分析雅各比。我们希望这项工作能促进在任意复杂的化学机制中使用分析雅各比。为了便于推广,我们将所提出的方法集成到了反应流求解器的开源套件 https://github.com/AMReX-Combustion/PelePhysics 中。
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