Analysis and modelling of PAHs in turbulent non-premixed jet flames

IF 6.2 2区 工程技术 Q2 ENERGY & FUELS
Combustion and Flame Pub Date : 2026-05-01 Epub Date: 2026-02-27 DOI:10.1016/j.combustflame.2026.114892
Geveen Arumapperuma, Antonio Attili
{"title":"Analysis and modelling of PAHs in turbulent non-premixed jet flames","authors":"Geveen Arumapperuma,&nbsp;Antonio Attili","doi":"10.1016/j.combustflame.2026.114892","DOIUrl":null,"url":null,"abstract":"<div><div>This study investigates the formation, evolution, and modelling of polycyclic aromatic hydrocarbons (PAH) using large-scale three-dimensional direct numerical simulations (DNS) of spatially evolving turbulent non-premixed ethylene/air flames. Finite rate chemistry is used with a detailed chemical mechanism for ethylene oxidation with naphthalene as the PAH species. Three cases are analysed: two at the same Reynolds number with different Damköhler numbers and one at a higher Reynolds number with the same Damköhler number as one of the lower Reynolds number cases. A strong correlation is observed between the mean PAH field and the mean scalar dissipation rate, while the correlation between the local instantaneous values is extremely weak. For a given streamwise location of the flame, if the mean scalar dissipation rate is the same between the simulations, the mean PAH concentration is also the same, irrespective of the Damköhler number. It was also shown that the mean scalar dissipation rate, conditioned on the mixture fraction, can be used to retrieve the PAH mass fraction accurately from a table build using steady flamelets. These observations suggest that highly fluctuating quantities like PAHs in turbulent flames, despite being uncorrelated to the local turbulent and mixing fields, are however related to the mean fields. Moreover, the PAH is found to be insensitive to the Reynolds number, as no significant difference in the PAH field can be observed between the two flames with different Reynolds numbers. An <em>a priori</em> analysis revealed that the PAH source terms deviate considerably from the steady flamelet solution and a linear scaling of the PAH consumption term based on the local PAH concentration leads to significant errors. In addition to the DNS, an LES with tabulated chemistry of the higher Reynolds number flame is performed for an <em>a posteriori</em> analysis of the PAH modelling errors. The PAH is modelled using a transport equation where the source term is read from a flamelet table. Two separate LESs are performed, one with a unity Lewis number flamelet table and the other with a table generated with mixture-averaged transport. Both LESs capture the spatial distribution of PAH with reasonable accuracy. However, the unity Lewis number LES significantly underpredicts the magnitude of PAH by about an order of magnitude. The non-unity Lewis number LES shows an improvement, albeit still underpredicting the DNS results. It is observed that the prediction errors are mostly associated with the errors in the PAH source terms from the flamelet model and highlights the need to improve the model. Finally, the idea of using the mean scalar dissipation to parametrise PAH in LES is tested <em>a posteriori</em> and it is found that this can be a viable approach.</div><div><strong>Novelty and significance statement</strong></div><div>A novel, large-scale direct numerical simulation dataset of a realistic flame configuration was generated. The detailed analysis of the data provided important insights into the fundamental nature of soot precursor evolution. The study revealed a strong correlation between the mean scalar dissipation rate and the mean PAH mass fraction, which can be leveraged to develop novel modelling strategies. The study also showed that PAH is insensitive to the Reynolds number. It also highlighted the limitations of current PAH modelling strategies and identified areas where improvements are needed. The dataset provides a valuable resource to extend the understanding of turbulent non-premixed flames and to support the development of reduced-order models for large-eddy simulations or Reynolds-averaged Navier-Stokes simulations.</div></div>","PeriodicalId":280,"journal":{"name":"Combustion and Flame","volume":"287 ","pages":"Article 114892"},"PeriodicalIF":6.2000,"publicationDate":"2026-05-01","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/S0010218026001288","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2026/2/27 0:00:00","PubModel":"Epub","JCR":"Q2","JCRName":"ENERGY & FUELS","Score":null,"Total":0}
引用次数: 0

Abstract

This study investigates the formation, evolution, and modelling of polycyclic aromatic hydrocarbons (PAH) using large-scale three-dimensional direct numerical simulations (DNS) of spatially evolving turbulent non-premixed ethylene/air flames. Finite rate chemistry is used with a detailed chemical mechanism for ethylene oxidation with naphthalene as the PAH species. Three cases are analysed: two at the same Reynolds number with different Damköhler numbers and one at a higher Reynolds number with the same Damköhler number as one of the lower Reynolds number cases. A strong correlation is observed between the mean PAH field and the mean scalar dissipation rate, while the correlation between the local instantaneous values is extremely weak. For a given streamwise location of the flame, if the mean scalar dissipation rate is the same between the simulations, the mean PAH concentration is also the same, irrespective of the Damköhler number. It was also shown that the mean scalar dissipation rate, conditioned on the mixture fraction, can be used to retrieve the PAH mass fraction accurately from a table build using steady flamelets. These observations suggest that highly fluctuating quantities like PAHs in turbulent flames, despite being uncorrelated to the local turbulent and mixing fields, are however related to the mean fields. Moreover, the PAH is found to be insensitive to the Reynolds number, as no significant difference in the PAH field can be observed between the two flames with different Reynolds numbers. An a priori analysis revealed that the PAH source terms deviate considerably from the steady flamelet solution and a linear scaling of the PAH consumption term based on the local PAH concentration leads to significant errors. In addition to the DNS, an LES with tabulated chemistry of the higher Reynolds number flame is performed for an a posteriori analysis of the PAH modelling errors. The PAH is modelled using a transport equation where the source term is read from a flamelet table. Two separate LESs are performed, one with a unity Lewis number flamelet table and the other with a table generated with mixture-averaged transport. Both LESs capture the spatial distribution of PAH with reasonable accuracy. However, the unity Lewis number LES significantly underpredicts the magnitude of PAH by about an order of magnitude. The non-unity Lewis number LES shows an improvement, albeit still underpredicting the DNS results. It is observed that the prediction errors are mostly associated with the errors in the PAH source terms from the flamelet model and highlights the need to improve the model. Finally, the idea of using the mean scalar dissipation to parametrise PAH in LES is tested a posteriori and it is found that this can be a viable approach.
Novelty and significance statement
A novel, large-scale direct numerical simulation dataset of a realistic flame configuration was generated. The detailed analysis of the data provided important insights into the fundamental nature of soot precursor evolution. The study revealed a strong correlation between the mean scalar dissipation rate and the mean PAH mass fraction, which can be leveraged to develop novel modelling strategies. The study also showed that PAH is insensitive to the Reynolds number. It also highlighted the limitations of current PAH modelling strategies and identified areas where improvements are needed. The dataset provides a valuable resource to extend the understanding of turbulent non-premixed flames and to support the development of reduced-order models for large-eddy simulations or Reynolds-averaged Navier-Stokes simulations.
湍流非预混射流火焰中多环芳烃的分析与建模
本研究利用空间演化湍流非预混乙烯/空气火焰的大尺度三维直接数值模拟(DNS)研究了多环芳烃(PAH)的形成、演化和建模。用有限速率化学对以萘为多环芳烃的乙烯氧化进行了详细的化学机理研究。分析了三种情况:两种是相同雷诺数,但Damköhler数不同;一种是较高雷诺数,但Damköhler数相同,但雷诺数较低。平均多环芳烃场与平均标量耗散率有较强的相关性,而局部瞬时值的相关性极弱。对于给定的火焰流向位置,如果模拟之间的平均标量耗散率相同,则平均多环芳烃浓度也相同,而与Damköhler数字无关。结果还表明,以混合分数为条件的平均标量耗散率可以准确地从使用稳定小火焰建立的表中检索多环芳烃的质量分数。这些观测结果表明,湍流火焰中的多环芳烃等高度波动的量,尽管与局部湍流和混合场无关,但与平均场有关。此外,发现多环芳烃对雷诺数不敏感,在不同雷诺数的两种火焰中,多环芳烃场没有显著差异。先验分析表明,多环芳烃源项与稳定的火焰溶液存在较大偏差,基于局部多环芳烃浓度的多环芳烃消耗项线性缩放导致显著误差。除了DNS之外,还对高雷诺数火焰的化学表进行了LES,用于对多环芳烃建模误差进行后验分析。PAH使用传输方程建模,其中源项是从flamelet表读取的。执行了两个独立的LESs,一个使用统一Lewis数火焰表,另一个使用混合平均传输生成的表。两种LESs都能以合理的精度捕获多环芳烃的空间分布。然而,统一路易斯数LES显著低估了多环芳烃的大小约一个数量级。非统一刘易斯数LES显示了改进,尽管仍然低估了DNS结果。结果表明,预测误差主要与火焰模型中多环芳烃源项的误差有关,并强调了改进模型的必要性。最后,对利用平均标量耗散来参数化LES中多环芳烃的想法进行了后验检验,发现这是一种可行的方法。新颖性和意义声明生成了一种新颖的、大规模的真实火焰形态直接数值模拟数据集。对这些数据的详细分析为了解煤烟前驱体演化的基本性质提供了重要的见解。该研究揭示了平均标量耗散率与平均多环芳烃质量分数之间的强相关性,这可以用于开发新的建模策略。研究还表明,多环芳烃对雷诺数不敏感。它还强调了目前多环芳烃建模战略的局限性,并确定了需要改进的领域。该数据集为扩展对湍流非预混火焰的理解提供了宝贵的资源,并支持开发用于大涡模拟或reynolds -average Navier-Stokes模拟的降阶模型。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
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.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信
小红书