M. Vilespy , A. Aniello , D. Laera , T. Poinsot , T. Schuller , L. Selle
{"title":"非预混双旋流氢火焰NOx排放来源分析","authors":"M. Vilespy , A. Aniello , D. Laera , T. Poinsot , T. Schuller , L. Selle","doi":"10.1016/j.combustflame.2024.113925","DOIUrl":null,"url":null,"abstract":"<div><div>The mechanisms of NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> formation in swirled hydrogen-air flames are investigated with Large Eddy Simulations (LES). Two operating conditions, A (3 kW) and L (9 kW), are considered. Flame A is M-shaped with a first diffusion-controlled front attached to the hydrogen injector rim and a second flame front burning hydrogen and vitiated recirculating air. Flame L, instead, is lifted and stabilized as a V-flame at the bottom of the central recirculation zone. Flame L also features a diffusion reaction layer in the central recirculation zone with partially premixed wings that develop along the inner shear layer above the injector. It is shown that the central diffusion front is common to both operating points and plays an essential role in the global NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> emissions of the burner for both operating conditions. A comparison between flamelets extracted from 3D simulations and results obtained with one-dimensional strained flames shows that strain plays an essential role in the production rate of NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> for all zones. In both flames, nitrous oxides are mainly produced in the central diffusion front. The high temperature in this front favor NO formation through the thermal NO pathway, which is strongly dominant over the other ones. Nevertheless, the central diffusion front of the lifted flame (L) is submitted to a higher strain rate than the attached flame (A), which leads to lower temperature and consequently to a smaller NO production. Interestingly, it is demonstrated that these differences can be predicted using one-dimensional strained diffusion flames. These simulations emphasize the key role of strain rate to control NO emissions in hydrogen non-premixed flames, and show that NO emissions are not necessarily increased by diffusion hydrogen flames attached to the injector lips.</div><div><strong>Novelty and significance statement</strong></div><div>NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> emissions are a key factor in designing future hydrogen gas turbines. While it is commonly assumed that diffusion-dominated flames produce high NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> levels, this paper shows that hydrogen swirled burners can achieve low NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> emissions even in a diffusion regime. Strained laminar diffusion hydrogen flames are known to limit NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> production, and this study extends that understanding to turbulent swirled flames. The main source of NO is not the typical diffusion ‘H<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>/air’ flame (Flame I) near the injector, but rather a secondary ‘H<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>/lean burnt gas’ diffusion layer (Flame II), stabilized downstream in the central recirculation zone. Simulations indicate that Flame I experiences high strain rates, while Flame II is nearly unstrained. This suggests that low NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> levels can be achieved by controlling the flow and local strain rates so that burning in a diffusion mode might not be a showstopper for future H<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span> engines.</div></div>","PeriodicalId":280,"journal":{"name":"Combustion and Flame","volume":"273 ","pages":"Article 113925"},"PeriodicalIF":6.2000,"publicationDate":"2025-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Analysis of the origin of NOx emissions in non premixed dual swirl hydrogen flames\",\"authors\":\"M. Vilespy , A. Aniello , D. Laera , T. Poinsot , T. Schuller , L. Selle\",\"doi\":\"10.1016/j.combustflame.2024.113925\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>The mechanisms of NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> formation in swirled hydrogen-air flames are investigated with Large Eddy Simulations (LES). Two operating conditions, A (3 kW) and L (9 kW), are considered. Flame A is M-shaped with a first diffusion-controlled front attached to the hydrogen injector rim and a second flame front burning hydrogen and vitiated recirculating air. Flame L, instead, is lifted and stabilized as a V-flame at the bottom of the central recirculation zone. Flame L also features a diffusion reaction layer in the central recirculation zone with partially premixed wings that develop along the inner shear layer above the injector. It is shown that the central diffusion front is common to both operating points and plays an essential role in the global NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> emissions of the burner for both operating conditions. A comparison between flamelets extracted from 3D simulations and results obtained with one-dimensional strained flames shows that strain plays an essential role in the production rate of NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> for all zones. In both flames, nitrous oxides are mainly produced in the central diffusion front. The high temperature in this front favor NO formation through the thermal NO pathway, which is strongly dominant over the other ones. Nevertheless, the central diffusion front of the lifted flame (L) is submitted to a higher strain rate than the attached flame (A), which leads to lower temperature and consequently to a smaller NO production. Interestingly, it is demonstrated that these differences can be predicted using one-dimensional strained diffusion flames. These simulations emphasize the key role of strain rate to control NO emissions in hydrogen non-premixed flames, and show that NO emissions are not necessarily increased by diffusion hydrogen flames attached to the injector lips.</div><div><strong>Novelty and significance statement</strong></div><div>NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> emissions are a key factor in designing future hydrogen gas turbines. While it is commonly assumed that diffusion-dominated flames produce high NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> levels, this paper shows that hydrogen swirled burners can achieve low NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> emissions even in a diffusion regime. Strained laminar diffusion hydrogen flames are known to limit NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> production, and this study extends that understanding to turbulent swirled flames. The main source of NO is not the typical diffusion ‘H<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>/air’ flame (Flame I) near the injector, but rather a secondary ‘H<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>/lean burnt gas’ diffusion layer (Flame II), stabilized downstream in the central recirculation zone. Simulations indicate that Flame I experiences high strain rates, while Flame II is nearly unstrained. This suggests that low NO<span><math><msub><mrow></mrow><mrow><mi>x</mi></mrow></msub></math></span> levels can be achieved by controlling the flow and local strain rates so that burning in a diffusion mode might not be a showstopper for future H<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span> engines.</div></div>\",\"PeriodicalId\":280,\"journal\":{\"name\":\"Combustion and Flame\",\"volume\":\"273 \",\"pages\":\"Article 113925\"},\"PeriodicalIF\":6.2000,\"publicationDate\":\"2025-03-01\",\"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/S0010218024006345\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2025/1/8 0:00:00\",\"PubModel\":\"Epub\",\"JCR\":\"Q2\",\"JCRName\":\"ENERGY & FUELS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Combustion and Flame","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0010218024006345","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/1/8 0:00:00","PubModel":"Epub","JCR":"Q2","JCRName":"ENERGY & FUELS","Score":null,"Total":0}
Analysis of the origin of NOx emissions in non premixed dual swirl hydrogen flames
The mechanisms of NO formation in swirled hydrogen-air flames are investigated with Large Eddy Simulations (LES). Two operating conditions, A (3 kW) and L (9 kW), are considered. Flame A is M-shaped with a first diffusion-controlled front attached to the hydrogen injector rim and a second flame front burning hydrogen and vitiated recirculating air. Flame L, instead, is lifted and stabilized as a V-flame at the bottom of the central recirculation zone. Flame L also features a diffusion reaction layer in the central recirculation zone with partially premixed wings that develop along the inner shear layer above the injector. It is shown that the central diffusion front is common to both operating points and plays an essential role in the global NO emissions of the burner for both operating conditions. A comparison between flamelets extracted from 3D simulations and results obtained with one-dimensional strained flames shows that strain plays an essential role in the production rate of NO for all zones. In both flames, nitrous oxides are mainly produced in the central diffusion front. The high temperature in this front favor NO formation through the thermal NO pathway, which is strongly dominant over the other ones. Nevertheless, the central diffusion front of the lifted flame (L) is submitted to a higher strain rate than the attached flame (A), which leads to lower temperature and consequently to a smaller NO production. Interestingly, it is demonstrated that these differences can be predicted using one-dimensional strained diffusion flames. These simulations emphasize the key role of strain rate to control NO emissions in hydrogen non-premixed flames, and show that NO emissions are not necessarily increased by diffusion hydrogen flames attached to the injector lips.
Novelty and significance statement
NO emissions are a key factor in designing future hydrogen gas turbines. While it is commonly assumed that diffusion-dominated flames produce high NO levels, this paper shows that hydrogen swirled burners can achieve low NO emissions even in a diffusion regime. Strained laminar diffusion hydrogen flames are known to limit NO production, and this study extends that understanding to turbulent swirled flames. The main source of NO is not the typical diffusion ‘H/air’ flame (Flame I) near the injector, but rather a secondary ‘H/lean burnt gas’ diffusion layer (Flame II), stabilized downstream in the central recirculation zone. Simulations indicate that Flame I experiences high strain rates, while Flame II is nearly unstrained. This suggests that low NO levels can be achieved by controlling the flow and local strain rates so that burning in a diffusion mode might not be a showstopper for future H engines.
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.