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Morphological characteristics of non-vertical turbulent jet flames: Experimental investigation and analytical model 非垂直湍流喷射火焰的形态特征:实验研究与分析模型
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-07-01 DOI: 10.1016/j.combustflame.2024.113589
Shixiang Liu , Michael A. Delichatsios , Longhua Hu

Non-vertical turbulent non-premixed jet flame occur in combustion systems and by accidental release of fuels caused fires. Understanding the combustion dynamics of these asymmetric diffusion jet flames is needed to characterize the flame morphology and entrainment, which is a foundation for further detailed analysis of the physics and implications. This paper investigates experimentally and theoretically the flame morphological characteristics of non-vertical turbulent jets at both positive- and negative inclined angles in a systematic way. A total of 168 experimental cases were considered involving various initial fuel flow rates, inclined angles and nozzle diameters. Dimensional analysis was performed taking into account the controlling parameters of the physical mechanisms, namely the momentum flux, the fuel mass flow rate, the flame buoyancy, the stoichiometric ratio and the jet initial inclined angle, which together determine a characteristic length scale and a characteristic volumetric flow rate. These two characteristic parameters provide successful non-dimensional correlations for the location of the flame tip. A new integral model was also developed physically considering the momentum and continuity equations along the trajectory to predict the flame tip, as well as the lowest point for negative inclined jets. By comparing the experimental correlations with numerical prediction, the effective air entrainment coefficients were derived for different jet initial inclined angles, which showed little change with inclined angle from positive to negative, but the constant relating the average values to the integrals of the (Gaussian) radial profiles decreased as the initial angle decreased from positive to negative. This change is related to the variation of the profile properties normal to the trajectory as well as to mass detrainment laterally escaping from the jet flame especially for negative inclined angles. Finally, the local Richardson number and the flame lowest point for negative inclined angles was numerically predicted and compared well with the experimental results.

非垂直湍流非预混合喷射火焰发生在燃烧系统中,也会因燃料意外释放而引起火灾。需要了解这些非对称扩散喷射火焰的燃烧动力学,以确定火焰形态和夹带的特征,这是进一步详细分析其物理和影响的基础。本文从实验和理论两方面系统地研究了正倾角和负倾角非垂直湍流射流的火焰形态特征。共考虑了 168 个实验案例,涉及不同的初始燃料流速、倾斜角度和喷嘴直径。在进行尺寸分析时,考虑了物理机制的控制参数,即动量通量、燃料质量流量、火焰浮力、化学计量比和射流初始倾斜角,这些参数共同决定了特征长度尺度和特征容积流量。这两个特征参数为焰尖位置提供了成功的非尺寸相关性。此外,还开发了一个新的积分模型,该模型在物理上考虑了沿轨迹的动量方程和连续性方程,以预测焰尖以及负倾斜喷流的最低点。通过将实验相关性与数值预测进行比较,得出了不同喷流初始倾斜角度下的有效空气夹带系数,结果表明,倾斜角度从正到负变化不大,但当初始角度从正到负减小时,与(高斯)径向剖面积分平均值相关的常数减小。这种变化与轨迹法线剖面特性的变化以及从喷射火焰横向逃逸的质量分离有关,特别是在负倾角情况下。最后,对负倾角的局部理查森数和火焰最低点进行了数值预测,并与实验结果进行了很好的比较。
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引用次数: 0
High-frequency hydrogen combustion dynamics driven by local flame displacement and multidimensional thermoacoustic interactions 局部火焰位移和多维热声相互作用驱动的高频氢气燃烧动力学
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-06-28 DOI: 10.1016/j.combustflame.2024.113592
Dohyung Park, Jaehyun Park, Kyu Tae Kim

Knowledge of the underlying physical mechanisms responsible for the triggering of high-frequency transverse combustion dynamics is of fundamental importance in the development of heavy-duty gas turbine combustors, aircraft engine afterburners, and bipropellant liquid rocket engines. Detailed information about three-dimensional thermoacoustic interactions and local flame dynamics, however, remains largely unknown and unanticipated, mainly because high-amplitude transverse mode instabilities are challenging to excite and detect in well-controlled sub-scale laboratory environments. To overcome this impasse, here we exploit a spatially tailored rectangular injector assembly consisting of ten equidistant horizontal slit nozzles to eliminate the complications of out-of-plane flame dynamics characterization. A total of 56 datasets of self-induced instabilities were acquired over a wide range of operating conditions to understand spatiotemporal phase dynamics and important mode shapes, in conjunction with 2D Rayleigh angle reconstruction and phase-resolved OH PLIF-based local flame front identification. Experimentally, we show that high-frequency transverse instabilities are excited only under high temperature and high thermal power conditions, manifested as non-evanescent pressure fluctuations at 6.50 kHz strongly coupled to the second-order tangential mode of the rectangular combustion chamber. Two vertically-oriented pressure nodal planes and the characteristic phase transition perpendicular to the horizontal slit injector direction are accurately measured and reconfirmed by Helmholtz simulations in terms of their interpositions and spatial orientation. Remarkably, the periodic formation of co-propagating coherent structures and concomitant local flame displacement/pinch-off are revealed to play an important role in driving the high-frequency hydrogen combustion dynamics.

了解引发高频横向燃烧动力学的基本物理机制对于重型燃气涡轮燃烧器、飞机发动机后燃烧器和双推进液体火箭发动机的开发至关重要。然而,有关三维热声相互作用和局部火焰动力学的详细信息在很大程度上仍然是未知和不可预期的,这主要是因为在控制良好的亚尺度实验室环境中激发和检测高振幅横模不稳定性具有挑战性。为了打破这一僵局,我们在这里利用了空间定制的矩形喷射器组件,该组件由十个等距水平狭缝喷嘴组成,消除了平面外火焰动力学特征描述的复杂性。在广泛的工作条件下,我们共获取了 56 个自诱发不稳定性数据集,结合二维瑞利角重构和基于相位分辨 OH PLIF 的局部火焰前沿识别,了解了时空相位动力学和重要模态形状。实验结果表明,高频横向不稳定性仅在高温和高热功率条件下才会被激发,表现为 6.50 kHz 的非渐变压力波动与矩形燃烧室的二阶切向模强耦合。两个垂直方向的压力节点平面和垂直于水平狭缝喷射器方向的特征相变得到了精确测量,并通过亥姆霍兹模拟重新确认了它们的相互位置和空间方向。值得注意的是,共传播相干结构的周期性形成和随之而来的局部火焰位移/夹断在驱动高频氢气燃烧动力学方面发挥了重要作用。
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引用次数: 0
Thermal behaviors of coal particles in an impinging entrained-flow gasifier: Char oxidation 煤颗粒在撞击内流气化炉中的热行为:炭氧化
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-06-28 DOI: 10.1016/j.combustflame.2024.113575
Yue Wang , Yan Gong , Hantao Lu , Qinghua Guo , Guangsuo Yu

The thermal behaviors of high-temperature particle (HTP) and low-temperature particle (LTP) are investigated based on the bench-scale impinging entrained-flow coal-water slurry (CWS) gasification experimental platform with a modified visualization system. The size and velocity distribution of both particles, and the evolution of HTP are analyzed through the algorithmic and precise processing of the image sequences. In addition, in-situ temperature diagnosis of the particles during the reaction process were realized. The typical evolution process and the temperature of HTP in char oxidation stage are obtained. The results show that the concentration of HTP in the gasifier is greater than LTP, but the particle size is relatively small. Particles moving at the low speed (0–2 m/s) account for the largest proportion of both HTP and LTP. The char oxidation process lasts over 300 ms and can be divided into three reaction stages. During the reaction, the peak temperature at the center of the particle can reach more than 2000 K. The average temperature of the particles gradually increased, reaching a peak in reaction stage II (1500 K) followed by a gradual decrease. The particle temperature is affected by O/C and is prone to experience swelling and bubbling phenomena during char oxidation.

基于台架规模的冲击内流水煤浆(CWS)气化实验平台和改进的可视化系统,研究了高温颗粒(HTP)和低温颗粒(LTP)的热行为。通过对图像序列进行算法和精确处理,分析了两种颗粒的尺寸和速度分布以及低温颗粒的演变过程。此外,还实现了反应过程中颗粒的原位温度诊断。获得了炭氧化阶段 HTP 的典型演化过程和温度。结果表明,气化炉中 HTP 的浓度大于 LTP,但粒径相对较小。在低速(0-2 m/s)运动的颗粒中,HTP 和 LTP 所占比例最大。炭氧化过程持续时间超过 300 毫秒,可分为三个反应阶段。在反应过程中,颗粒中心的峰值温度可达 2000 K 以上,颗粒的平均温度逐渐升高,在反应第二阶段达到峰值(1500 K),随后逐渐降低。颗粒温度受 O/C 的影响,在炭氧化过程中容易出现膨胀和气泡现象。
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引用次数: 0
Cause-and-effect chain analysis of combustion cyclic variability in a spark-ignition engine using large-eddy simulation, Part II: Origins of flow variations from intake 利用大涡流模拟对火花点火发动机燃烧周期变化的因果链分析,第二部分:进气流量变化的起源
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-06-28 DOI: 10.1016/j.combustflame.2024.113565
Zhihao Ding, Karine Truffin, Stéphane Jay

In this work, the phenomenon of cycle-to-cycle variability (CCV) of combustion in a spark ignition engine is investigated to give a deeper understanding of CCV generation. The main objective is to localize within the cylinder and all along the engine cycle the flow variabilites and identify some driving mechanisms originating in the flow structures and leading to combustion variabilites. In Part I , the application of empirical mode decomposition methods combined with topology-based techniques to the LES flow results allowed the extraction of the large-scale flow motion from the small-scale turbulence and the follow-up of their evolution during compression stroke [1]. A link was then established between the combustion process and the tumble formation and destabilization near BDC. In the present paper, the overall tumble motion development during compression and intake strokes is quantitatively analyzed, and links are built between different engine phases to establish the cause-and-effect chain. Other CCV factors, such as spray injection and exhaust gas recirculation, were not included in the current study. However, the developed methodology for in-cylinder flow analysis could be used in studies on other engine configurations to improve the development of engine designs.

Novelty and significance statement

In this work, the cycle-to-cycle variability (CCV) of combustion in a spark ignition engine is investigated to give a deeper understanding of CCV generation. The present study focuses on CCV caused by the stochastic nature of internal turbulent flow structures. LES approach is chosen due to its ability to capture CCV, and advanced flow analysis tools are developed and applied to LES results to characterize instantaneous flow structures of different scales in the three-dimensional domain and separately quantify their impacts on combustion.

A first important finding is that flow-wall interactions near BDC determine the tumble evolution.

A second novelty is the characterization of several 3D dominant flow interactions during intake yielding large-scale flow variability.

A third novelty and important finding is that links are found between the flow organization during intake, the tumble development, and destabilization during early compression and the combustion. Throughout our analyses starting from the spark timing and going back to the early intake phase, a cause-and-effect chain is finally established between the development of in-cylinder flow and the combustion variability.

在这项工作中,对火花点火发动机中燃烧的周期变异(CCV)现象进行了研究,以深入了解 CCV 的产生。主要目的是定位气缸内和发动机整个循环过程中的流动变异,并确定一些源于流动结构并导致燃烧变异的驱动机制。在第一部分中,将经验模式分解方法与基于拓扑的技术相结合应用于 LES 流动结果,可以从小规模湍流中提取大规模流动运动,并跟踪其在压缩冲程中的演变[1]。随后,在燃烧过程与 BDC 附近的翻滚形成和失稳之间建立了联系。本文定量分析了压缩冲程和进气冲程中的整体翻滚运动发展,并在发动机不同阶段之间建立联系,以建立因果关系链。本研究不包括其他 CCV 因素,如喷射和废气再循环。然而,所开发的气缸内流动分析方法可用于其他发动机配置的研究,以改进发动机设计的开发。本研究的重点是由内部湍流结构的随机性引起的 CCV。由于 LES 能够捕捉 CCV,因此选择了 LES 方法,并开发了先进的流动分析工具,将其应用于 LES 结果,以表征三维域中不同尺度的瞬时流动结构,并分别量化其对燃烧的影响。第三个新颖而重要的发现是,我们发现进气过程中的流动组织、翻滚发展以及早期压缩和燃烧过程中的不稳定之间存在联系。我们的分析从火花定时开始,一直追溯到进气早期阶段,最终在缸内流动的发展和燃烧变化之间建立了因果关系链。
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引用次数: 0
On dynamics of gasless combustion in slowly varying periodic media 论缓慢变化的周期性介质中的无气燃烧动力学
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-06-27 DOI: 10.1016/j.combustflame.2024.113573
Amanda Matson , Leonid Kagan , Claude-Michel Brauner , Gregory Sivashinsky , Peter V. Gordon

In this paper we consider a classical model of gasless combustion in a one dimensional formulation under the assumption of ignition temperature kinetics. We study the propagation of flame fronts in this model when the initial distribution of the solid fuel is a spatially periodic function that varies on a large scale. It is shown that in certain parametric regimes the model supports periodic traveling fronts. An accurate asymptotic formula for the velocity of the flame front is derived and studied. The stability of periodic fronts is also explored, and a critical condition in terms of parameters of the problem is derived. It is also shown that the instability of periodic fronts, in certain parametric regimes, results in a propagation-extinction-conduction-reignition pattern which is studied numerically.

Novelty and significance statement: This work provides a closed form asymptotic description of periodic traveling fronts in a gasless combustion model with step-wise ignition temperature kinetics with a slowly varying concentration field. The stability analysis is performed, and the range of applicability of asymptotic formulas is given. A new propagation-extinction-conduction-reignition regime is identified. This regime emerges exclusively due to periodicity of the concentration field.

在本文中,我们考虑了一个经典的无气燃烧模型,该模型是在点火温度动力学假设下的一维模型。我们研究了当固体燃料的初始分布是一个在大尺度上变化的空间周期函数时,火焰前沿在该模型中的传播。结果表明,在某些参数情况下,该模型支持周期性的行进前沿。推导并研究了火焰前沿速度的精确渐近公式。此外,还探讨了周期性前沿的稳定性,并得出了问题参数的临界条件。研究还表明,在某些参数条件下,周期性前沿的不稳定性会导致传播-熄灭-传导-复燃模式,并对该模式进行了数值研究:这项工作提供了一个无气燃烧模型中周期性行进前沿的封闭形式渐近描述,该模型具有步进式点火温度动力学和缓慢变化的浓度场。进行了稳定性分析,并给出了渐近公式的适用范围。确定了一个新的传播-熄灭-传导-复燃机制。该机制的出现完全是由于浓度场的周期性。
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引用次数: 0
Roles of fuel composition on the ignition process of endothermic hydrocarbons 燃料成分对内热碳氢化合物点火过程的影响
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-06-26 DOI: 10.1016/j.combustflame.2024.113591
Hao Liu , Shu Zheng , Xinyi Chen , Tipeng Wang , Ran Sui , Qiang Lu

Due to the characteristics of heat absorption and decomposition, endothermic hydrocarbon fuels (EHFs) have been widely used in scramjets for thermal protection and heat recirculation. The understanding of ignition characteristics of EHFs is of great importance for their safe and efficient utilization. In this paper, the ignition processes of EHFs were numerically simulated at atmospheric pressure and with an initial temperature of 500 K. Three different ignition stages were identified based on the chemical heat release and flame kernel propagation. A 3-component kerosene surrogate model composed of n-dodecane, methyl cyclohexane and m-xylene was adopted, as well as the corresponding chemical kinetic model with 369 species and 2691 reactions. Results showed that the discrepant decomposition characteristics of n-alkanes and cycloalkanes affected the chemical heat release and propagation during the ignition process. Two-stage exothermic characteristic was observed in the time evolutions of chemical heat release rate and fuel decomposition. The mass production of molecules and accumulation of radicals dominated the first and second exothermic peaks, respectively. Furthermore, the minimum ignition energies (MIEs) of EHFs with various methyl cyclohexane were determined to quantify the effect of fuel composition on ignition performance. Characteristically, the MIE dramatically decreased from 10.2 to 2.15 mJ when 20% n-dodecane was replaced by methyl cyclohexane. However, it was slightly increased as methyl cyclohexane continued to increase. Analyses from both physical and chemical aspects were conducted to elaborate the dependence of MIE on fuel composition. The dominant effects of flame-dynamic and chemical effects on different ignition stages were analysed. The faster propagation speed and stronger endothermic ability of methyl cyclohexane led to the nonlinear variation of MIEs. The results in this study provide useful guidance for composition optimization and safety evaluation of EHFs.

由于具有吸热和分解的特性,内热碳氢化合物燃料(EHFs)已被广泛用于扰流喷气式飞机的热保护和热再循环。了解 EHFs 的点火特性对其安全高效利用具有重要意义。本文对 EHFs 在大气压力和 500 K 初始温度下的点火过程进行了数值模拟。采用了由正十二烷、甲基环己烷和间二甲苯组成的三组分煤油代用模型,以及相应的化学动力学模型,其中包含 369 个物种和 2691 个反应。结果表明,正构烷烃和环构烷烃的不同分解特性影响了点火过程中化学热的释放和传播。在化学放热率和燃料分解的时间演化过程中,观察到了两阶段放热特征。分子的大量产生和自由基的积累分别主导了第一和第二放热峰。此外,还测定了含有不同甲基环己烷的 EHFs 的最小点火能(MIEs),以量化燃料成分对点火性能的影响。从特征上看,当 20% 的正十二烷被甲基环己烷取代时,MIE 从 10.2 mJ 急剧下降到 2.15 mJ。不过,随着甲基环己烷的不断增加,MIE 也略有增加。从物理和化学两方面进行了分析,以阐述 MIE 与燃料成分的关系。分析了火焰动力学效应和化学效应对不同点火阶段的主要影响。甲基环己烷的传播速度更快、内热能力更强,这导致了 MIE 的非线性变化。这项研究的结果为超高频的成分优化和安全评估提供了有用的指导。
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引用次数: 0
Effect of 2-butanone addition to ethylene fuel on soot formation in counterflow diffusion flames using newly proposed soot model 利用新提出的烟尘模型,在乙烯燃料中添加 2-丁酮对逆流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 : 2024-06-26 DOI: 10.1016/j.combustflame.2024.113572
Subrat Garnayak, Hrishikesh Gadgil, Sudarshan Kumar

An improved consistent soot model is proposed and applied to evaluate the effect of 2-butanone addition (10 % to 50 % on a volume basis represented as case 1 to case 5) to ethylene fuel on soot formation using a counterflow burner configuration. The predictive capability of the suggested soot model is verified by assessing its performance against existing experimental data on soot formation (SF) configuration-type ethylene counterflow flames at diverse strain rates and various fuel additives. The proposed soot model comprises 55 inception reactions with temperature-dependent collision efficiency and 10 condensation reactions from 10 PAH species (from naphthalene to larger PAHs up to coronene), including modified HACA surface growth and oxidation reactions. 2-butanone is produced as a byproduct during the pyrolysis of biomass and the microbiological fermentation of agricultural waste. It holds various benefits as a prospective biofuel for spark ignition (SI) engines. Limited information exists regarding its sooting characteristics due to a lack of available soot measurements. The simulations are conducted for the soot formation (SF) type counterflow flames with a fixed fuel and oxidizer jet velocity. The proposed soot model can effectively replicate both the qualitative and quantitative aspects of the experimental trends and shows a better agreement than the existing models available in the literature. The soot volume fraction (SVF) and the particle number density (PND) decrease with increasing the 2-butanone concentration in the binary fuel mixture. The PAH concentration decreases with increasing 2-butanone addition in the fuel mixture. The peak SVF and the maximum temperature are reduced by ∼22.7 % and ∼3.6 %, with a 40 % increase in the 2-butanone portion in the fuel mixture from case 1 to case 5. Increasing the 2-butanone content in the fuel mixture decreases the inception rate, HACA rate, and condensation rate while it increases the oxidation rate.

本文提出了一种改进的一致烟尘模型,并将其应用于评估使用逆流燃烧器配置的乙烯燃料中添加 2-丁酮(体积百分比为 10% 至 50%,分别代表情况 1 至情况 5)对烟尘形成的影响。通过评估建议烟尘模型在不同应变率和各种燃料添加剂条件下的性能,并根据现有的烟尘形成(SF)配置型乙烯逆流火焰实验数据,验证了该模型的预测能力。所提出的烟尘模型包括 55 个起始反应(碰撞效率随温度变化)和 10 种多环芳烃(从萘到较大的多环芳烃直至冠烯)的 10 个缩合反应,其中包括改进的 HACA 表面生长和氧化反应。2-butanone 是生物质热解和农业废弃物微生物发酵过程中产生的副产品。作为一种可用于火花点火(SI)发动机的生物燃料,它具有多种优点。由于缺乏烟尘测量数据,有关其烟尘特性的信息非常有限。我们对固定燃料和氧化剂喷射速度的烟尘形成(SF)型逆流火焰进行了模拟。所提出的烟尘模型能有效复制实验趋势的定性和定量方面,与文献中现有的模型相比显示出更好的一致性。烟尘体积分数(SVF)和颗粒数密度(PND)随着二元燃料混合物中 2-丁酮浓度的增加而降低。多环芳烃浓度随着燃料混合物中 2-丁酮添加量的增加而降低。从情况 1 到情况 5,随着燃料混合物中 2-丁酮含量增加 40%,峰值 SVF 和最高温度分别降低了 22.7% 和 3.6%。增加燃料混合物中的 2-丁酮含量会降低萌发率、HACA 率和冷凝率,同时增加氧化率。
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引用次数: 0
Cause-and-effect chain analysis of combustion cyclic variability in a spark-ignition engine using large-eddy simulation, Part I: From tumble compression to flame initiation 利用大涡流模拟对火花点火发动机燃烧周期变化的因果链分析,第一部分:从翻滚压缩到火焰启动
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-06-24 DOI: 10.1016/j.combustflame.2024.113566
Zhihao Ding , Karine Truffin, Stéphane Jay

Understanding, modeling, and reducing the cycle-to-cycle variability (CCV) of combustion in internal combustion engines (ICE) is a critical challenge to design engines of high efficiency and low emissions. A high level of CCV may contribute to partial burn, misfire, and knock in extreme engine cycles, which affects engine performance and eventually damages the engine. The origins of CCV have been studied both experimentally and numerically, and the variability of in-cylinder aerodynamics is recognized as one of the most important sources of CCV. However, a detailed and quantitative explanation of how in-cylinder flow CCV is generated is not yet clear. The objective of the present study is to develop a methodology to localize inside the chamber of a spark-ignition engine (SIE) the origins of flow variabilities and to identify some driving mechanisms leading to combustion variabilities. Multi-cycle wall-modeled large-eddy simulations (LES) for the TU Darmstadt optical engine under fired conditions are performed using the CFD solver Converge 3.0. The evolution of organized large-scale structures and the small-scale turbulence of the in-cylinder flow are analyzed using a developed methodology that includes the empirical mode decomposition (EMD) method adapted for 2D and 3D flow fields, and a vortex identification tool Γ3p. The contributions of different parts of the flow to CCV are quantified. In Part I of this work, the LES framework is validated against experimental data, and CCV of large-scale structures is characterized at spark timing. In Part II, the overall flow development during compression and intake strokes are quantitatively analyzed, and links are built between different engine phases to establish the cause-and-effect chain. Other CCV factors, such as spray injection and exhaust gas recirculation, are not included in the current study. However, the developed methodology for in-cylinder flow analysis could be used in studies on other engine configurations to improve the development of engine designs.

Novelty and significance statement

In this work, the cycle-to-cycle variability (CCV) of combustion in a spark ignition engine is investigated to give a deeper understanding of CCV generation. The present study focuses on CCV caused by the stochastic nature of internal turbulent flow structures. LES approach is chosen due to its ability to capture CCV. The LES methodology was validated in a motored case in Ding et al. (2023). In the present study, it is validated in a reactive case against experimental in-cylinder pressures and velocity fields.

A first novelty is the application of EMD methods combined with topology-based techniques to reactive LES results to characterize flow structures of different scales in the three-dimensional domain and to quantify separately their impacts on combustion.

A second n

要设计出高效率、低排放的发动机,了解、模拟和减少内燃机(ICE)燃烧的循环变异性(CCV)是一项严峻的挑战。高水平的 CCV 可能会在极端发动机循环中导致部分燃烧、失火和爆震,从而影响发动机性能并最终损坏发动机。人们通过实验和数值方法对 CCV 的起源进行了研究,缸内空气动力学的可变性被认为是 CCV 的最重要来源之一。然而,关于气缸内气流 CCV 如何产生的详细定量解释尚不清楚。本研究的目的是开发一种方法,用于定位火花点火式发动机(SIE)燃烧室内流动变化的起源,并确定导致燃烧变化的一些驱动机制。使用 CFD 求解器 Converge 3.0 对达姆施塔特工业大学的光学发动机在点火条件下进行了多周期壁面建模大涡流模拟(LES)。该方法包括适用于二维和三维流场的经验模式分解(EMD)方法和涡流识别工具Γ3p。对流体不同部分对 CCV 的贡献进行了量化。在本研究的第一部分,根据实验数据对 LES 框架进行了验证,并对火花定时的大型结构的 CCV 进行了描述。在第二部分中,定量分析了压缩和进气冲程期间的整体流动发展,并在发动机的不同阶段之间建立联系,以建立因果关系链。目前的研究不包括其他 CCV 因素,如喷射和废气再循环。然而,所开发的气缸内流动分析方法可用于其他发动机配置的研究,以改进发动机设计的开发。本研究的重点是由内部湍流结构的随机性引起的 CCV。选择 LES 方法是因为它能够捕捉 CCV。在 Ding 等人(2023 年)的研究中,LES 方法已在发动机情况下得到验证。本研究的第一个创新点是将 EMD 方法与基于拓扑的技术相结合,应用于反应式 LES 结果,以描述三维域中不同尺度的流动结构,并分别量化其对燃烧的影响。第二个新颖之处和重要发现是在燃烧速度与 BDC 附近的翻滚形成和不稳定性之间建立了联系。通过我们在第一和第二部分中的分析,从火花点火时间开始,追溯到进气早期阶段,最终在气缸内流动的发展和燃烧变化之间建立了因果关系链。
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引用次数: 0
Experimental study of nitric oxide distributions in non-premixed and premixed ammonia/hydrogen-air counterflow flames 非预混合和预混合氨气/氢气逆流火焰中一氧化氮分布的实验研究
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-06-24 DOI: 10.1016/j.combustflame.2024.113556
Hao Tang , Zeinab Al Hadi , Thibault F. Guiberti , Wenting Sun , Gaetano Magnotti

This study reports an experimental investigation of quantitative Nitric Oxide (NO) distribution in both premixed and non-premixed NH3/H2-air flames using a counterflow burner at atmospheric pressure. One-dimensional (1D) NO laser-induced fluorescence (LIF) spectroscopy and Raman/Rayleigh spectroscopy were conducted to accurately resolve the quantitative 1D NO profile in terms of mixture fraction, temperature, and physical space. We calibrated a saturated NO-LIF model in 5 premixed lean H2/N2/NO-air flames with different seeded NO levels in a McKenna burner and validated its accuracy in three H2N2NO-air counterflow diffusion flames. The overall uncertainty of NO quantification was less than90 ppm. Our measurements were compared with simulations using different ammonia chemical kinetic models, revealing that current models have over 30% uncertainty in predicting peak NO concentrations (mole fraction) in 1D non-premixed and premixed flames and over 100% uncertainty in lower temperature regions. In premixed flames, measured NO concentrations fell within the intermediate range of current chemical kinetic models at lean and stoichiometric conditions, but were lower than the models at rich conditions. In non-premixed flames, all models overestimated the peak NO concentrations by more than 1000 ppm. It is noted that the measured peak NO concentrations increased with higher NH3/H2 ratios (from 4/6 to 8/2), strain rates (from 80 to 140 1/s), and N2 dilution ratios in a 1:1 NH3/H2 mixture (from 0 to 30%). Although most models could qualitatively predict the trends, they were inaccurate in quantifying NO. Additionally, the measured width of the NO profile in mixture fraction space expanded with increasing NH3/H2 ratio, N2 dilution ratio, and strain rate. While models could qualitatively predict this behavior, they consistently underestimated NO in the fuel-rich, lower-temperature region, resulting in a narrower NO profile width. The Manna model showed a better prediction of NO distribution in the fuel rich portion of non-premixed flames, accounting for NH3NO interactions at lower temperatures. These findings highlight the critical need to improve models to accurately predict NO concentrations in ammonia-containing flames and their behavior in fuel rich regions.

本研究报告了在大气压力下使用逆流燃烧器对预混合和非预混合 NH3/H2- 空气火焰中一氧化氮(NO)定量分布的实验研究。我们采用了一维(1D)NO 激光诱导荧光(LIF)光谱和拉曼/雷利光谱,以准确解析一维 NO 在混合物组分、温度和物理空间方面的定量分布。我们在麦肯纳燃烧器中的 5 个具有不同 NO 种子水平的预混合贫 H2/N2/NO-air 火焰中校准了饱和 NO-LIF 模型,并在 3 个 H2N2NO-air 逆流扩散火焰中验证了其准确性。氮氧化物定量的总体不确定性小于 90 ppm。我们将测量结果与使用不同氨化学动力学模型的模拟结果进行了比较,结果表明,目前的模型在预测一维非预混合和预混合火焰中的 NO 浓度峰值(摩尔分数)时,不确定性超过 30%,而在较低温度区域,不确定性超过 100%。在预混火焰中,在贫气和化学计量条件下,测得的氮氧化物浓度在当前化学动力学模型的中间范围内,但在富气条件下低于模型。在非预混合火焰中,所有模型都高估了 NO 的峰值浓度,高出 1000 ppm 以上。值得注意的是,随着 NH3/H2 比率(从 4/6 到 8/2)、应变速率(从 80 到 140 1/s)和 1:1 NH3/H2 混合气中 N2 稀释比(从 0 到 30%)的提高,测得的 NO 峰值浓度也在增加。虽然大多数模型可以定性地预测趋势,但它们在量化 NO 方面并不准确。此外,随着 NH3/H2 比率、N2 稀释比率和应变速率的增加,在混合分数空间中测得的 NO 曲线宽度也在扩大。虽然模型可以定性地预测这种行为,但它们始终低估了富燃料、低温区域的 NO,导致 NO 剖面宽度变窄。Manna 模型能更好地预测非预混火焰中富含燃料部分的 NO 分布,并考虑到 NH3NO 在较低温度下的相互作用。这些发现突出表明,亟需改进模型,以准确预测含氨火焰中的 NO 浓度及其在富燃料区的行为。
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引用次数: 0
Thermal radiation and soot in buoyant turbulent diffusion flames under different oxygen concentrations: Measurements and implications to radiation modeling 不同氧气浓度下浮力湍流扩散火焰中的热辐射和烟尘:测量结果及其对辐射建模的影响
IF 5.8 2区 工程技术 Q2 ENERGY & FUELS Pub Date : 2024-06-24 DOI: 10.1016/j.combustflame.2024.113587
Gang Xiong, Dong Zeng, Yi Wang

To develop and validate numerical models for sooty fires, we have established a dataset of the thermal radiation and soot in 15 kW buoyant turbulent ethylene flames. The flames are stabilized on a water-cooled round burner with a 15.2 cm outer diameter (D) and 13.7 cm inner diameter at three oxygen concentrations (OC) of 15.2 %, 16.8 %, and 20.9 %. A two-color optical probe is used to measure the spectral radiative intensities at two wavelengths, from which soot volume fraction and temperature are determined. The overall mean soot volume fractions are consistent with results from laser induced incandescence and laser extinction measurements. For a given OC, the mean soot temperature and volume fraction conditioned on the radiative intensity greater than a threshold value (instrumental detection limit) are relatively independent of spatial location. When OC decreases from 20.9 % to 15.2 %, the conditional mean soot volume fraction decreases by a factor of two. However, the conditional mean soot temperature at different locations and OCs are within a narrow range (with a standard deviation of only 22 K). The effect of detection limit is discussed, and the results show that the correlation between soot volume fraction and temperature is weak with a sufficiently low detection limit. Based on the experimental findings, a simplified model for the turbulence-radiation interaction (TRI) is proposed for application in the numerical modeling of soot radiation. The model approximates the turbulent closure term for radiation by taking advantage of the fact that the soot temperature has a relatively unchanged mean value and a narrow quasi-normal distribution within the buoyant turbulent flame, regardless of the spatial location and oxygen concentration. Therefore, the soot emission power can be directly calculated from the mean soot volume fraction and conditional mean soot temperature in a decoupled manner.

为了开发和验证烟尘火灾的数值模型,我们建立了 15 千瓦浮力湍流乙烯火焰的热辐射和烟尘数据集。火焰稳定在一个外径(D)为 15.2 厘米、内径为 13.7 厘米的水冷圆形燃烧器上,氧气浓度(OC)分别为 15.2%、16.8% 和 20.9%。使用双色光学探针测量两个波长的光谱辐射强度,并据此确定烟尘体积分数和温度。总体平均烟尘体积分数与激光诱导炽化和激光消光测量的结果一致。对于给定的 OC,在辐射强度大于阈值(仪器检测极限)的条件下,平均烟尘温度和体积分数与空间位置相对无关。当 OC 从 20.9% 下降到 15.2% 时,条件平均烟尘体积分数下降了 2 倍。然而,不同地点和不同 OC 的条件平均烟尘温度范围很窄(标准偏差仅为 22 K)。讨论了检测限的影响,结果表明,在检测限足够低的情况下,烟尘体积分数与温度之间的相关性很弱。根据实验结果,提出了一个简化的湍流-辐射相互作用(TRI)模型,用于烟尘辐射的数值建模。该模型利用烟尘温度在浮力湍流火焰中具有相对不变的平均值和窄的准正态分布(与空间位置和氧气浓度无关)这一事实,对辐射的湍流闭合项进行了近似。因此,烟尘发射功率可以直接从平均烟尘体积分数和条件平均烟尘温度中脱钩计算出来。
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引用次数: 0
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Combustion and Flame
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