Influences of excess air coefficient on combustion and emission performance of diesel pilot ignition natural gas engine by coupling computational fluid dynamics with reduced chemical kinetic model
•Chemical mechanism was introduced to study λ ’s effect on natural gas-diesel engine.•Each combustion stage of natural gas-diesel engine was quantitatively analyzed.•The higher λ leads the heat release rate to shoot up earlier.•The 10–50% and 50–90% combustion duration become longer as λ increases f...
Gespeichert in:
Veröffentlicht in: | Energy conversion and management 2019-05, Vol.187, p.283-296 |
---|---|
Hauptverfasser: | , , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 296 |
---|---|
container_issue | |
container_start_page | 283 |
container_title | Energy conversion and management |
container_volume | 187 |
creator | Shu, Jun Fu, Jianqin Liu, Jingping Wang, Shuqian Yin, Yanshan Deng, Banglin Becker, Sid Martin |
description | •Chemical mechanism was introduced to study λ ’s effect on natural gas-diesel engine.•Each combustion stage of natural gas-diesel engine was quantitatively analyzed.•The higher λ leads the heat release rate to shoot up earlier.•The 10–50% and 50–90% combustion duration become longer as λ increases from 1.2.•The maximum nitrogen oxide emissions appear near the λ of 1.1.
In the presented study, the influence of lean-burn on combustion and emission performance of diesel pilot ignition natural gas engine was investigated by using the method of computational fluid dynamics coupling with the reduced chemical kinetic model. Based on bench tested results, the computational fluid dynamics model was validated in four typical conditions, and then it was used for the simulation at different excess air coefficient. Due to the visibility of computational fluid dynamics results, the combustion medium process and emissions medium products were obtained, which then were used to explain the influence mechanism of excess air coefficient. The simulated results show that, under 50% load, the maximum cylinder pressure becomes larger and the start of combustion is advanced when the excess air coefficient increases from 1.0 to 1.5, and the maximum advance of the start of combustion reaches 9.5 °CA. Nevertheless, under 100% load, the start of combustion is advanced first and then retarded. Meanwhile, the higher the excess air coefficient is, the earlier the heat release rate shoots up. When the excess air coefficient increases from 1.2, the 10–50%, 50–90% and 10–90% combustion duration become longer. The nitrogen oxide emission increases as the excess air coefficient rises from 1.0 to 1.1 but decreases if it continues to increase. The unburned methane emission decreases first and then increases with the increase of the excess air coefficient. Nevertheless, at 1500 rpm and full load, the unburned methane emission shoots up as the excess air coefficient changes from 1.3 to 1.5 and the maximum difference of unburned methane emission reaches 3233 ppm. |
doi_str_mv | 10.1016/j.enconman.2019.03.047 |
format | Article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_journals_2237862471</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0196890419303450</els_id><sourcerecordid>2237862471</sourcerecordid><originalsourceid>FETCH-LOGICAL-c340t-29a9d84afbfb3b409771e876c40142e004fe499f90a6626118ae180590687eef3</originalsourceid><addsrcrecordid>eNqFkc-O1DAMxiMEEsPCK6BInFucNJs2N9CKPyutxGX3HKWpM5uhTUqSAvN-PBgpA2dOseXPP9v5CHnNoGXA5NtTi8HGsJjQcmCqha4F0T8hBzb0quGc90_JoRZkMygQz8mLnE8A0F2DPJBft8HNWwVgptFR_FmDTI1P1EZ0zluPodAYarqMWy6-hiZMFBef856smFxMdbjFHTB5zDjT1c-xUH8M_k9HMGVLZqZHkymGow9Ix3NFbuvsw3Fnr1sxu7SK6j5-otM5mMXbTH_48kgTTpvFidrHOthW0dfKKN7SJU44vyTPnJkzvvr7XpGHjx_ubz43d18-3d68v2tsJ6A0XBk1DcK40Y3dKED1PcOhl1YAExwBhEOhlFNgpOSSscEgG-BagRx6RNddkTcX7pritw1z0ae4pbpz1px3_SC56FlVyYvKpphzQqfX5BeTzpqB3h3TJ_3PMb07pqHT1bHa-O7SiPWG7x6Tzvv317t9Qlv0FP3_EL8BFWKoGQ</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2237862471</pqid></control><display><type>article</type><title>Influences of excess air coefficient on combustion and emission performance of diesel pilot ignition natural gas engine by coupling computational fluid dynamics with reduced chemical kinetic model</title><source>ScienceDirect Journals (5 years ago - present)</source><creator>Shu, Jun ; Fu, Jianqin ; Liu, Jingping ; Wang, Shuqian ; Yin, Yanshan ; Deng, Banglin ; Becker, Sid Martin</creator><creatorcontrib>Shu, Jun ; Fu, Jianqin ; Liu, Jingping ; Wang, Shuqian ; Yin, Yanshan ; Deng, Banglin ; Becker, Sid Martin</creatorcontrib><description>•Chemical mechanism was introduced to study λ ’s effect on natural gas-diesel engine.•Each combustion stage of natural gas-diesel engine was quantitatively analyzed.•The higher λ leads the heat release rate to shoot up earlier.•The 10–50% and 50–90% combustion duration become longer as λ increases from 1.2.•The maximum nitrogen oxide emissions appear near the λ of 1.1.
In the presented study, the influence of lean-burn on combustion and emission performance of diesel pilot ignition natural gas engine was investigated by using the method of computational fluid dynamics coupling with the reduced chemical kinetic model. Based on bench tested results, the computational fluid dynamics model was validated in four typical conditions, and then it was used for the simulation at different excess air coefficient. Due to the visibility of computational fluid dynamics results, the combustion medium process and emissions medium products were obtained, which then were used to explain the influence mechanism of excess air coefficient. The simulated results show that, under 50% load, the maximum cylinder pressure becomes larger and the start of combustion is advanced when the excess air coefficient increases from 1.0 to 1.5, and the maximum advance of the start of combustion reaches 9.5 °CA. Nevertheless, under 100% load, the start of combustion is advanced first and then retarded. Meanwhile, the higher the excess air coefficient is, the earlier the heat release rate shoots up. When the excess air coefficient increases from 1.2, the 10–50%, 50–90% and 10–90% combustion duration become longer. The nitrogen oxide emission increases as the excess air coefficient rises from 1.0 to 1.1 but decreases if it continues to increase. The unburned methane emission decreases first and then increases with the increase of the excess air coefficient. Nevertheless, at 1500 rpm and full load, the unburned methane emission shoots up as the excess air coefficient changes from 1.3 to 1.5 and the maximum difference of unburned methane emission reaches 3233 ppm.</description><identifier>ISSN: 0196-8904</identifier><identifier>EISSN: 1879-2227</identifier><identifier>DOI: 10.1016/j.enconman.2019.03.047</identifier><language>eng</language><publisher>Oxford: Elsevier Ltd</publisher><subject>Aerodynamics ; Ceramics industry ; Chemical kinetic model ; Coefficients ; Combustion ; Computational fluid dynamics ; Computer applications ; Computer simulation ; Coupling ; Cylinders ; Diesel ; Diesel engines ; Emission analysis ; Emissions ; Excess air coefficient ; Fluid dynamics ; Full load ; Heat release rate ; Heat transfer ; Hydrodynamics ; Ignition ; Methane ; Natural gas ; Natural gas industry ; Nitrogen oxides ; Organic chemistry ; Shoots ; Visibility</subject><ispartof>Energy conversion and management, 2019-05, Vol.187, p.283-296</ispartof><rights>2019 Elsevier Ltd</rights><rights>Copyright Elsevier Science Ltd. May 1, 2019</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c340t-29a9d84afbfb3b409771e876c40142e004fe499f90a6626118ae180590687eef3</citedby><cites>FETCH-LOGICAL-c340t-29a9d84afbfb3b409771e876c40142e004fe499f90a6626118ae180590687eef3</cites><orcidid>0000-0002-4004-7730</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.enconman.2019.03.047$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3550,27924,27925,45995</link.rule.ids></links><search><creatorcontrib>Shu, Jun</creatorcontrib><creatorcontrib>Fu, Jianqin</creatorcontrib><creatorcontrib>Liu, Jingping</creatorcontrib><creatorcontrib>Wang, Shuqian</creatorcontrib><creatorcontrib>Yin, Yanshan</creatorcontrib><creatorcontrib>Deng, Banglin</creatorcontrib><creatorcontrib>Becker, Sid Martin</creatorcontrib><title>Influences of excess air coefficient on combustion and emission performance of diesel pilot ignition natural gas engine by coupling computational fluid dynamics with reduced chemical kinetic model</title><title>Energy conversion and management</title><description>•Chemical mechanism was introduced to study λ ’s effect on natural gas-diesel engine.•Each combustion stage of natural gas-diesel engine was quantitatively analyzed.•The higher λ leads the heat release rate to shoot up earlier.•The 10–50% and 50–90% combustion duration become longer as λ increases from 1.2.•The maximum nitrogen oxide emissions appear near the λ of 1.1.
In the presented study, the influence of lean-burn on combustion and emission performance of diesel pilot ignition natural gas engine was investigated by using the method of computational fluid dynamics coupling with the reduced chemical kinetic model. Based on bench tested results, the computational fluid dynamics model was validated in four typical conditions, and then it was used for the simulation at different excess air coefficient. Due to the visibility of computational fluid dynamics results, the combustion medium process and emissions medium products were obtained, which then were used to explain the influence mechanism of excess air coefficient. The simulated results show that, under 50% load, the maximum cylinder pressure becomes larger and the start of combustion is advanced when the excess air coefficient increases from 1.0 to 1.5, and the maximum advance of the start of combustion reaches 9.5 °CA. Nevertheless, under 100% load, the start of combustion is advanced first and then retarded. Meanwhile, the higher the excess air coefficient is, the earlier the heat release rate shoots up. When the excess air coefficient increases from 1.2, the 10–50%, 50–90% and 10–90% combustion duration become longer. The nitrogen oxide emission increases as the excess air coefficient rises from 1.0 to 1.1 but decreases if it continues to increase. The unburned methane emission decreases first and then increases with the increase of the excess air coefficient. Nevertheless, at 1500 rpm and full load, the unburned methane emission shoots up as the excess air coefficient changes from 1.3 to 1.5 and the maximum difference of unburned methane emission reaches 3233 ppm.</description><subject>Aerodynamics</subject><subject>Ceramics industry</subject><subject>Chemical kinetic model</subject><subject>Coefficients</subject><subject>Combustion</subject><subject>Computational fluid dynamics</subject><subject>Computer applications</subject><subject>Computer simulation</subject><subject>Coupling</subject><subject>Cylinders</subject><subject>Diesel</subject><subject>Diesel engines</subject><subject>Emission analysis</subject><subject>Emissions</subject><subject>Excess air coefficient</subject><subject>Fluid dynamics</subject><subject>Full load</subject><subject>Heat release rate</subject><subject>Heat transfer</subject><subject>Hydrodynamics</subject><subject>Ignition</subject><subject>Methane</subject><subject>Natural gas</subject><subject>Natural gas industry</subject><subject>Nitrogen oxides</subject><subject>Organic chemistry</subject><subject>Shoots</subject><subject>Visibility</subject><issn>0196-8904</issn><issn>1879-2227</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNqFkc-O1DAMxiMEEsPCK6BInFucNJs2N9CKPyutxGX3HKWpM5uhTUqSAvN-PBgpA2dOseXPP9v5CHnNoGXA5NtTi8HGsJjQcmCqha4F0T8hBzb0quGc90_JoRZkMygQz8mLnE8A0F2DPJBft8HNWwVgptFR_FmDTI1P1EZ0zluPodAYarqMWy6-hiZMFBef856smFxMdbjFHTB5zDjT1c-xUH8M_k9HMGVLZqZHkymGow9Ix3NFbuvsw3Fnr1sxu7SK6j5-otM5mMXbTH_48kgTTpvFidrHOthW0dfKKN7SJU44vyTPnJkzvvr7XpGHjx_ubz43d18-3d68v2tsJ6A0XBk1DcK40Y3dKED1PcOhl1YAExwBhEOhlFNgpOSSscEgG-BagRx6RNddkTcX7pritw1z0ae4pbpz1px3_SC56FlVyYvKpphzQqfX5BeTzpqB3h3TJ_3PMb07pqHT1bHa-O7SiPWG7x6Tzvv317t9Qlv0FP3_EL8BFWKoGQ</recordid><startdate>20190501</startdate><enddate>20190501</enddate><creator>Shu, Jun</creator><creator>Fu, Jianqin</creator><creator>Liu, Jingping</creator><creator>Wang, Shuqian</creator><creator>Yin, Yanshan</creator><creator>Deng, Banglin</creator><creator>Becker, Sid Martin</creator><general>Elsevier Ltd</general><general>Elsevier Science Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7ST</scope><scope>7TB</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>H8D</scope><scope>KR7</scope><scope>L7M</scope><scope>SOI</scope><orcidid>https://orcid.org/0000-0002-4004-7730</orcidid></search><sort><creationdate>20190501</creationdate><title>Influences of excess air coefficient on combustion and emission performance of diesel pilot ignition natural gas engine by coupling computational fluid dynamics with reduced chemical kinetic model</title><author>Shu, Jun ; Fu, Jianqin ; Liu, Jingping ; Wang, Shuqian ; Yin, Yanshan ; Deng, Banglin ; Becker, Sid Martin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c340t-29a9d84afbfb3b409771e876c40142e004fe499f90a6626118ae180590687eef3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Aerodynamics</topic><topic>Ceramics industry</topic><topic>Chemical kinetic model</topic><topic>Coefficients</topic><topic>Combustion</topic><topic>Computational fluid dynamics</topic><topic>Computer applications</topic><topic>Computer simulation</topic><topic>Coupling</topic><topic>Cylinders</topic><topic>Diesel</topic><topic>Diesel engines</topic><topic>Emission analysis</topic><topic>Emissions</topic><topic>Excess air coefficient</topic><topic>Fluid dynamics</topic><topic>Full load</topic><topic>Heat release rate</topic><topic>Heat transfer</topic><topic>Hydrodynamics</topic><topic>Ignition</topic><topic>Methane</topic><topic>Natural gas</topic><topic>Natural gas industry</topic><topic>Nitrogen oxides</topic><topic>Organic chemistry</topic><topic>Shoots</topic><topic>Visibility</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Shu, Jun</creatorcontrib><creatorcontrib>Fu, Jianqin</creatorcontrib><creatorcontrib>Liu, Jingping</creatorcontrib><creatorcontrib>Wang, Shuqian</creatorcontrib><creatorcontrib>Yin, Yanshan</creatorcontrib><creatorcontrib>Deng, Banglin</creatorcontrib><creatorcontrib>Becker, Sid Martin</creatorcontrib><collection>CrossRef</collection><collection>Environment Abstracts</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Environment Abstracts</collection><jtitle>Energy conversion and management</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Shu, Jun</au><au>Fu, Jianqin</au><au>Liu, Jingping</au><au>Wang, Shuqian</au><au>Yin, Yanshan</au><au>Deng, Banglin</au><au>Becker, Sid Martin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Influences of excess air coefficient on combustion and emission performance of diesel pilot ignition natural gas engine by coupling computational fluid dynamics with reduced chemical kinetic model</atitle><jtitle>Energy conversion and management</jtitle><date>2019-05-01</date><risdate>2019</risdate><volume>187</volume><spage>283</spage><epage>296</epage><pages>283-296</pages><issn>0196-8904</issn><eissn>1879-2227</eissn><abstract>•Chemical mechanism was introduced to study λ ’s effect on natural gas-diesel engine.•Each combustion stage of natural gas-diesel engine was quantitatively analyzed.•The higher λ leads the heat release rate to shoot up earlier.•The 10–50% and 50–90% combustion duration become longer as λ increases from 1.2.•The maximum nitrogen oxide emissions appear near the λ of 1.1.
In the presented study, the influence of lean-burn on combustion and emission performance of diesel pilot ignition natural gas engine was investigated by using the method of computational fluid dynamics coupling with the reduced chemical kinetic model. Based on bench tested results, the computational fluid dynamics model was validated in four typical conditions, and then it was used for the simulation at different excess air coefficient. Due to the visibility of computational fluid dynamics results, the combustion medium process and emissions medium products were obtained, which then were used to explain the influence mechanism of excess air coefficient. The simulated results show that, under 50% load, the maximum cylinder pressure becomes larger and the start of combustion is advanced when the excess air coefficient increases from 1.0 to 1.5, and the maximum advance of the start of combustion reaches 9.5 °CA. Nevertheless, under 100% load, the start of combustion is advanced first and then retarded. Meanwhile, the higher the excess air coefficient is, the earlier the heat release rate shoots up. When the excess air coefficient increases from 1.2, the 10–50%, 50–90% and 10–90% combustion duration become longer. The nitrogen oxide emission increases as the excess air coefficient rises from 1.0 to 1.1 but decreases if it continues to increase. The unburned methane emission decreases first and then increases with the increase of the excess air coefficient. Nevertheless, at 1500 rpm and full load, the unburned methane emission shoots up as the excess air coefficient changes from 1.3 to 1.5 and the maximum difference of unburned methane emission reaches 3233 ppm.</abstract><cop>Oxford</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.enconman.2019.03.047</doi><tpages>14</tpages><orcidid>https://orcid.org/0000-0002-4004-7730</orcidid></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0196-8904 |
ispartof | Energy conversion and management, 2019-05, Vol.187, p.283-296 |
issn | 0196-8904 1879-2227 |
language | eng |
recordid | cdi_proquest_journals_2237862471 |
source | ScienceDirect Journals (5 years ago - present) |
subjects | Aerodynamics Ceramics industry Chemical kinetic model Coefficients Combustion Computational fluid dynamics Computer applications Computer simulation Coupling Cylinders Diesel Diesel engines Emission analysis Emissions Excess air coefficient Fluid dynamics Full load Heat release rate Heat transfer Hydrodynamics Ignition Methane Natural gas Natural gas industry Nitrogen oxides Organic chemistry Shoots Visibility |
title | Influences of excess air coefficient on combustion and emission performance of diesel pilot ignition natural gas engine by coupling computational fluid dynamics with reduced chemical kinetic model |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-07T00%3A27%3A56IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Influences%20of%20excess%20air%20coefficient%20on%20combustion%20and%20emission%20performance%20of%20diesel%20pilot%20ignition%20natural%20gas%20engine%20by%20coupling%20computational%20fluid%20dynamics%20with%20reduced%20chemical%20kinetic%20model&rft.jtitle=Energy%20conversion%20and%20management&rft.au=Shu,%20Jun&rft.date=2019-05-01&rft.volume=187&rft.spage=283&rft.epage=296&rft.pages=283-296&rft.issn=0196-8904&rft.eissn=1879-2227&rft_id=info:doi/10.1016/j.enconman.2019.03.047&rft_dat=%3Cproquest_cross%3E2237862471%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2237862471&rft_id=info:pmid/&rft_els_id=S0196890419303450&rfr_iscdi=true |