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key: GV58WNFN
data:
  {"key":"GV58WNFN","version":38,"data":{"key":"GV58WNFN","version":38,"itemType":"webpage","title":"Available Input Datasets - MUSICA - wiki.ucar.edu","creators":[],"abstractNote":"","websiteTitle":"","websiteType":"","date":"","shortTitle":"","url":"https://wiki.ucar.edu/display/MUSICA/Available+Input+Datasets","accessDate":"2022-04-27T02:24:21Z","language":"","rights":"","extra":"","tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T02:24:21Z","dateModified":"2022-04-27T02:24:21Z"}}


key: 689PRS6Z
data:
  {"key":"689PRS6Z","version":36,"data":{"key":"689PRS6Z","version":36,"itemType":"computerProgram","title":"MUSICA Tutorial","creators":[],"abstractNote":"","seriesTitle":"","versionNumber":"","date":"2022-03-06T01:02:49Z","system":"","place":"","company":"National Center for Atmospheric Research","programmingLanguage":"Jupyter Notebook","ISBN":"","shortTitle":"","url":"https://github.com/NCAR/musica-tutorial/blob/87e8adbfd57cd27f9b31552f480fc251c988fa91/functions/Plot_2D.py","rights":"Apache-2.0","archive":"","archiveLocation":"","libraryCatalog":"GitHub","callNumber":"","accessDate":"2022-04-27T02:08:21Z","extra":"original-date: 2021-10-27T21:23:49Z","deleted":1,"tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T02:08:21Z","dateModified":"2022-04-27T02:08:21Z"}}


key: D5VH9H67
data:
  {"key":"D5VH9H67","version":34,"data":{"key":"D5VH9H67","version":34,"itemType":"computerProgram","title":"MUSICA Tutorial","creators":[],"abstractNote":"","seriesTitle":"","versionNumber":"","date":"2022-03-06T01:02:49Z","system":"","place":"","company":"National Center for Atmospheric Research","programmingLanguage":"Jupyter Notebook","ISBN":"","shortTitle":"","url":"https://github.com/NCAR/musica-tutorial/blob/87e8adbfd57cd27f9b31552f480fc251c988fa91/timeseries.ipynb","rights":"Apache-2.0","archive":"","archiveLocation":"","libraryCatalog":"GitHub","callNumber":"","accessDate":"2022-04-27T02:05:32Z","extra":"original-date: 2021-10-27T21:23:49Z","tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T02:05:32Z","dateModified":"2022-04-27T02:05:32Z"}}


key: J6QY6Z4D
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  {"key":"J6QY6Z4D","version":33,"data":{"key":"J6QY6Z4D","version":33,"itemType":"webpage","title":"cesm.ucar.edu Modeling CESM Presentation","creators":[],"abstractNote":"","websiteTitle":"","websiteType":"","date":"","shortTitle":"","url":"https://www.cesm.ucar.edu/events/workshops/ws.2016/presentations/ccwg/tilmes.pdf","accessDate":"2022-04-27T01:38:05Z","language":"","rights":"","extra":"","tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T01:38:05Z","dateModified":"2022-04-27T01:41:00Z"}}


key: GSFIUBZU
data:
  {"key":"GSFIUBZU","version":32,"data":{"key":"GSFIUBZU","version":32,"itemType":"webpage","title":"A Methodology for Measuring Size-Dependent Chemical Composition of Ultrane Particles","creators":[],"abstractNote":"","websiteTitle":"","websiteType":"","date":"","shortTitle":"","url":"https://cfpub.epa.gov/ncer_abstracts/INDEX.cfm/fuseaction/display.pubFullText/publication_id/35598","accessDate":"2022-04-27T00:47:42Z","language":"","rights":"","extra":"","tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T00:47:42Z","dateModified":"2022-04-27T01:40:09Z"}}


key: SB2BWPZI
data:
  {"key":"SB2BWPZI","version":31,"data":{"key":"SB2BWPZI","version":31,"itemType":"journalArticle","title":"Characterization of organic aerosol across the global remote troposphere: a comparison of ATom measurements and global chemistry models","creators":[{"creatorType":"author","firstName":"Alma","lastName":"Hodzic"},{"creatorType":"author","firstName":"Pedro","lastName":"Campuzano-Jost"},{"creatorType":"author","firstName":"Huisheng","lastName":"Bian"},{"creatorType":"author","firstName":"Mian","lastName":"Chin"},{"creatorType":"author","firstName":"Peter R.","lastName":"Colarco"},{"creatorType":"author","firstName":"Douglas A.","lastName":"Day"},{"creatorType":"author","firstName":"Karl D.","lastName":"Froyd"},{"creatorType":"author","firstName":"Bernd","lastName":"Heinold"},{"creatorType":"author","firstName":"Duseong S.","lastName":"Jo"},{"creatorType":"author","firstName":"Joseph M.","lastName":"Katich"},{"creatorType":"author","firstName":"John K.","lastName":"Kodros"},{"creatorType":"author","firstName":"Benjamin A.","lastName":"Nault"},{"creatorType":"author","firstName":"Jeffrey R.","lastName":"Pierce"},{"creatorType":"author","firstName":"Eric","lastName":"Ray"},{"creatorType":"author","firstName":"Jacob","lastName":"Schacht"},{"creatorType":"author","firstName":"Gregory P.","lastName":"Schill"},{"creatorType":"author","firstName":"Jason C.","lastName":"Schroder"},{"creatorType":"author","firstName":"Joshua P.","lastName":"Schwarz"},{"creatorType":"author","firstName":"Donna T.","lastName":"Sueper"},{"creatorType":"author","firstName":"Ina","lastName":"Tegen"},{"creatorType":"author","firstName":"Simone","lastName":"Tilmes"},{"creatorType":"author","firstName":"Kostas","lastName":"Tsigaridis"},{"creatorType":"author","firstName":"Pengfei","lastName":"Yu"},{"creatorType":"author","firstName":"Jose L.","lastName":"Jimenez"}],"abstractNote":"Abstract. The spatial distribution and properties of submicron organic aerosol (OA)\nare among the key sources of uncertainty in our understanding of aerosol\neffects on climate. Uncertainties are particularly large over remote regions\nof the free troposphere and Southern Ocean, where very few data have been\navailable and where OA predictions from AeroCom Phase II global models span 2 to 3 orders of magnitude, greatly exceeding the model spread over\nsource regions. The (nearly) pole-to-pole vertical distribution of\nnon-refractory aerosols was measured with an aerosol mass spectrometer\nonboard the NASA DC-8 aircraft as part of the Atmospheric Tomography (ATom)\nmission during the Northern Hemisphere summer (August 2016) and winter\n(February 2017). This study presents the first extensive characterization of\nOA mass concentrations and their level of oxidation in the remote\natmosphere. OA and sulfate are the major contributors by mass to submicron\naerosols in the remote troposphere, together with sea salt in the marine\nboundary layer. Sulfate was dominant in the lower stratosphere. OA\nconcentrations have a strong seasonal and zonal variability, with the\nhighest levels measured in the lower troposphere in the summer and over the\nregions influenced by biomass burning from Africa (up to 10 µg sm−3). Lower concentrations (∼0.1–0.3 µg sm−3)\nare observed in the northern middle and high latitudes and very low\nconcentrations (<0.1 µg sm−3) in the southern middle and\nhigh latitudes. The ATom dataset is used to evaluate predictions of eight\ncurrent global chemistry models that implement a variety of commonly used\nrepresentations of OA sources and chemistry, as well as of the AeroCom-II\nensemble. The current model ensemble captures the average vertical and\nspatial distribution of measured OA concentrations, and the spread of the\nindividual models remains within a factor of 5. These results are\nsignificantly improved over the AeroCom-II model ensemble, which shows large\noverestimations over these regions. However, some of the improved agreement\nwith observations occurs for the wrong reasons, as models have the tendency\nto greatly overestimate the primary OA fraction and underestimate the\nsecondary fraction. Measured OA in the remote free troposphere is highly\noxygenated, with organic aerosol to organic carbon (OA ∕ OC) ratios of\n∼2.2–2.8, and is 30 %–60 % more oxygenated than in current\nmodels, which can lead to significant errors in OA concentrations. The\nmodel–measurement comparisons presented here support the concept of a more\ndynamic OA system as proposed by Hodzic et al. (2016), with enhanced removal\nof primary OA and a stronger production of secondary OA in global models\nneeded to provide better agreement with observations.","publicationTitle":"Atmospheric Chemistry and Physics","volume":"20","issue":"8","pages":"4607-4635","date":"2020-04-21","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Atmos. Chem. Phys.","language":"en","DOI":"10.5194/acp-20-4607-2020","ISSN":"1680-7324","shortTitle":"Characterization of organic aerosol across the global remote troposphere","url":"https://acp.copernicus.org/articles/20/4607/2020/","accessDate":"2022-04-27T01:38:59Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T01:38:59Z","dateModified":"2022-04-27T01:38:59Z"}}


key: QACV5FIU
data:
  {"key":"QACV5FIU","version":28,"data":{"key":"QACV5FIU","version":28,"itemType":"journalArticle","title":"Climate Forcing and Trends of Organic Aerosols in the Community Earth System Model (CESM2)","creators":[{"creatorType":"author","firstName":"S.","lastName":"Tilmes"},{"creatorType":"author","firstName":"A.","lastName":"Hodzic"},{"creatorType":"author","firstName":"L. K.","lastName":"Emmons"},{"creatorType":"author","firstName":"M. J.","lastName":"Mills"},{"creatorType":"author","firstName":"A.","lastName":"Gettelman"},{"creatorType":"author","firstName":"D. E.","lastName":"Kinnison"},{"creatorType":"author","firstName":"M.","lastName":"Park"},{"creatorType":"author","firstName":"J.-F.","lastName":"Lamarque"},{"creatorType":"author","firstName":"F.","lastName":"Vitt"},{"creatorType":"author","firstName":"M.","lastName":"Shrivastava"},{"creatorType":"author","firstName":"P.","lastName":"Campuzano-Jost"},{"creatorType":"author","firstName":"J. L.","lastName":"Jimenez"},{"creatorType":"author","firstName":"X.","lastName":"Liu"}],"abstractNote":"The Community Earth System Model version 2 (CESM2) includes three main atmospheric configurations: the Community Atmosphere Model version 6 (CAM6) with simplified chemistry and a simplified organic aerosol (OA) scheme, CAM6 with comprehensive tropospheric and stratospheric chemistry representation (CAM6-chem), and the Whole Atmosphere Community Climate Model version 6 (WACCM6). Both, CAM6-chem and WACCM6 include a more comprehensive secondary organic aerosols (SOA) approach using the Volatility Basis Set (VBS) scheme and prognostic stratospheric aerosols. This paper describes the different OA schemes available in the different atmospheric configurations of CESM2 and discusses differences in aerosol burden and resulting climate forcings. Derived OA burden and trends differ due to differences in OA formation using the different approaches. Regional differences in Aerosol Optical Depth with larger values using the comprehensive approach occur over SOA source regions. Stronger increasing SOA trends between 1960 and 2015 in WACCM6 compared to CAM6 are due to increasing biogenic emissions aligned with increasing surface temperatures. Using the comprehensive SOA approach further leads to improved comparisons to aircraft observations and SOA formation of ≈143 Tg/yr. We further use WACCM6 to identify source contributions of OA from biogenic, fossil fuel, and biomass burning emissions, to quantify SOA amounts and trends from these sources. Increasing SOA trends between 1960 and 2015 are the result of increasing biogenic emissions aligned with increasing surface temperatures. Biogenic emissions are at least two thirds of the total SOA burden. In addition, SOA source contributions from fossil fuel emissions become more important, with largest values over Southeast Asia. The estimated total anthropogenic forcing of OA in WACCM6 for 1995–2010 conditions is −0.43 W/m2, mostly from the aerosol direct effect.","publicationTitle":"Journal of Advances in Modeling Earth Systems","volume":"11","issue":"12","pages":"4323-4351","date":"2019","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"","language":"en","DOI":"10.1029/2019MS001827","ISSN":"1942-2466","shortTitle":"","url":"https://onlinelibrary.wiley.com/doi/abs/10.1029/2019MS001827","accessDate":"2022-04-27T01:13:25Z","archive":"","archiveLocation":"","libraryCatalog":"Wiley Online Library","callNumber":"","rights":"","extra":"_eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1029/2019MS001827","tags":[{"tag":"CESM2","type":1},{"tag":"WACCM6","type":1},{"tag":"organic aerosols","type":1}],"collections":[],"relations":{},"dateAdded":"2022-04-27T01:13:25Z","dateModified":"2022-04-27T01:13:25Z"}}


key: WZC2MAVR
data:
  {"key":"WZC2MAVR","version":27,"data":{"key":"WZC2MAVR","version":27,"itemType":"journalArticle","title":"Climate Forcing and Trends of Organic Aerosols in the Community Earth System Model (CESM2)","creators":[{"creatorType":"author","firstName":"S.","lastName":"Tilmes"},{"creatorType":"author","firstName":"A.","lastName":"Hodzic"},{"creatorType":"author","firstName":"L. K.","lastName":"Emmons"},{"creatorType":"author","firstName":"M. J.","lastName":"Mills"},{"creatorType":"author","firstName":"A.","lastName":"Gettelman"},{"creatorType":"author","firstName":"D. E.","lastName":"Kinnison"},{"creatorType":"author","firstName":"M.","lastName":"Park"},{"creatorType":"author","firstName":"J.‐F.","lastName":"Lamarque"},{"creatorType":"author","firstName":"F.","lastName":"Vitt"},{"creatorType":"author","firstName":"M.","lastName":"Shrivastava"},{"creatorType":"author","firstName":"P.","lastName":"Campuzano‐Jost"},{"creatorType":"author","firstName":"J. L.","lastName":"Jimenez"},{"creatorType":"author","firstName":"X.","lastName":"Liu"}],"abstractNote":"","publicationTitle":"Journal of Advances in Modeling Earth Systems","volume":"11","issue":"12","pages":"4323-4351","date":"12/2019","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"J. Adv. Model. Earth Syst.","language":"en","DOI":"10.1029/2019MS001827","ISSN":"1942-2466, 1942-2466","shortTitle":"","url":"https://onlinelibrary.wiley.com/doi/abs/10.1029/2019MS001827","accessDate":"2022-04-27T00:59:51Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","deleted":1,"tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T00:59:51Z","dateModified":"2022-04-27T00:59:51Z"}}


key: 22MRUMR2
data:
  {"key":"22MRUMR2","version":26,"data":{"key":"22MRUMR2","version":26,"itemType":"journalArticle","title":"The Chemistry Mechanism in the Community Earth System Model Version 2 (CESM2)","creators":[{"creatorType":"author","firstName":"Louisa K.","lastName":"Emmons"},{"creatorType":"author","firstName":"Rebecca H.","lastName":"Schwantes"},{"creatorType":"author","firstName":"John J.","lastName":"Orlando"},{"creatorType":"author","firstName":"Geoff","lastName":"Tyndall"},{"creatorType":"author","firstName":"Douglas","lastName":"Kinnison"},{"creatorType":"author","firstName":"Jean‐François","lastName":"Lamarque"},{"creatorType":"author","firstName":"Daniel","lastName":"Marsh"},{"creatorType":"author","firstName":"Michael J.","lastName":"Mills"},{"creatorType":"author","firstName":"Simone","lastName":"Tilmes"},{"creatorType":"author","firstName":"Charles","lastName":"Bardeen"},{"creatorType":"author","firstName":"Rebecca R.","lastName":"Buchholz"},{"creatorType":"author","firstName":"Andrew","lastName":"Conley"},{"creatorType":"author","firstName":"Andrew","lastName":"Gettelman"},{"creatorType":"author","firstName":"Rolando","lastName":"Garcia"},{"creatorType":"author","firstName":"Isobel","lastName":"Simpson"},{"creatorType":"author","firstName":"Donald R.","lastName":"Blake"},{"creatorType":"author","firstName":"Simone","lastName":"Meinardi"},{"creatorType":"author","firstName":"Gabrielle","lastName":"Pétron"}],"abstractNote":"","publicationTitle":"Journal of Advances in Modeling Earth Systems","volume":"12","issue":"4","pages":"","date":"04/2020","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"J. Adv. Model. Earth Syst.","language":"en","DOI":"10.1029/2019MS001882","ISSN":"1942-2466, 1942-2466","shortTitle":"","url":"https://onlinelibrary.wiley.com/doi/10.1029/2019MS001882","accessDate":"2022-04-27T00:59:51Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","deleted":1,"tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T00:59:51Z","dateModified":"2022-04-27T00:59:51Z"}}


key: RDNK57R8
data:
  {"key":"RDNK57R8","version":25,"data":{"key":"RDNK57R8","version":25,"itemType":"journalArticle","title":"NCAR Release of CAM‐SE in CESM2.0: A Reformulation of the Spectral Element Dynamical Core in Dry‐Mass Vertical Coordinates With Comprehensive Treatment of Condensates and Energy","creators":[{"creatorType":"author","firstName":"P. H.","lastName":"Lauritzen"},{"creatorType":"author","firstName":"R. D.","lastName":"Nair"},{"creatorType":"author","firstName":"A. R.","lastName":"Herrington"},{"creatorType":"author","firstName":"P.","lastName":"Callaghan"},{"creatorType":"author","firstName":"S.","lastName":"Goldhaber"},{"creatorType":"author","firstName":"J. M.","lastName":"Dennis"},{"creatorType":"author","firstName":"J. T.","lastName":"Bacmeister"},{"creatorType":"author","firstName":"B. E.","lastName":"Eaton"},{"creatorType":"author","firstName":"C. M.","lastName":"Zarzycki"},{"creatorType":"author","firstName":"Mark A.","lastName":"Taylor"},{"creatorType":"author","firstName":"P. A.","lastName":"Ullrich"},{"creatorType":"author","firstName":"T.","lastName":"Dubos"},{"creatorType":"author","firstName":"A.","lastName":"Gettelman"},{"creatorType":"author","firstName":"R. B.","lastName":"Neale"},{"creatorType":"author","firstName":"B.","lastName":"Dobbins"},{"creatorType":"author","firstName":"K. A.","lastName":"Reed"},{"creatorType":"author","firstName":"C.","lastName":"Hannay"},{"creatorType":"author","firstName":"B.","lastName":"Medeiros"},{"creatorType":"author","firstName":"J. J.","lastName":"Benedict"},{"creatorType":"author","firstName":"J. J.","lastName":"Tribbia"}],"abstractNote":"","publicationTitle":"Journal of Advances in Modeling Earth Systems","volume":"10","issue":"7","pages":"1537-1570","date":"07/2018","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"J. Adv. Model. Earth Syst.","language":"en","DOI":"10.1029/2017MS001257","ISSN":"1942-2466, 1942-2466","shortTitle":"NCAR Release of CAM‐SE in CESM2.0","url":"https://onlinelibrary.wiley.com/doi/10.1029/2017MS001257","accessDate":"2022-04-27T00:59:51Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T00:59:51Z","dateModified":"2022-04-27T00:59:51Z"}}


key: TPMX8CBX
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key: QPCFUA9A
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key: H4L7FRUI
data:
  {"key":"H4L7FRUI","version":23,"data":{"key":"H4L7FRUI","version":23,"itemType":"webpage","title":"Course environment","creators":[],"abstractNote":"","websiteTitle":"","websiteType":"","date":"","shortTitle":"","url":"https://geo-python-site.readthedocs.io/en/latest/lessons/L1/course-environment-components.html#interactive-code-cells","accessDate":"2022-04-27T00:44:03Z","language":"","rights":"","extra":"","deleted":1,"tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T00:44:03Z","dateModified":"2022-04-27T00:44:03Z"}}


key: NZIZX7XU
data:
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key: QYWGQX24
data:
  {"key":"QYWGQX24","version":48,"data":{"key":"QYWGQX24","version":48,"itemType":"journalArticle","title":"The Chemistry Mechanism in the Community Earth System Model Version 2 (CESM2)","creators":[{"creatorType":"author","firstName":"Louisa K.","lastName":"Emmons"},{"creatorType":"author","firstName":"Rebecca H.","lastName":"Schwantes"},{"creatorType":"author","firstName":"John J.","lastName":"Orlando"},{"creatorType":"author","firstName":"Geoff","lastName":"Tyndall"},{"creatorType":"author","firstName":"Douglas","lastName":"Kinnison"},{"creatorType":"author","firstName":"Jean‐François","lastName":"Lamarque"},{"creatorType":"author","firstName":"Daniel","lastName":"Marsh"},{"creatorType":"author","firstName":"Michael J.","lastName":"Mills"},{"creatorType":"author","firstName":"Simone","lastName":"Tilmes"},{"creatorType":"author","firstName":"Charles","lastName":"Bardeen"},{"creatorType":"author","firstName":"Rebecca R.","lastName":"Buchholz"},{"creatorType":"author","firstName":"Andrew","lastName":"Conley"},{"creatorType":"author","firstName":"Andrew","lastName":"Gettelman"},{"creatorType":"author","firstName":"Rolando","lastName":"Garcia"},{"creatorType":"author","firstName":"Isobel","lastName":"Simpson"},{"creatorType":"author","firstName":"Donald R.","lastName":"Blake"},{"creatorType":"author","firstName":"Simone","lastName":"Meinardi"},{"creatorType":"author","firstName":"Gabrielle","lastName":"Pétron"}],"abstractNote":"","publicationTitle":"Journal of Advances in Modeling Earth Systems","volume":"12","issue":"4","pages":"","date":"04/2020","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"J. Adv. Model. Earth Syst.","language":"en","DOI":"10.1029/2019MS001882","ISSN":"1942-2466, 1942-2466","shortTitle":"","url":"https://onlinelibrary.wiley.com/doi/10.1029/2019MS001882","accessDate":"2022-04-27T00:43:07Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","deleted":1,"tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T00:43:07Z","dateModified":"2022-04-27T00:43:07Z"}}


key: QD3YARXP
data:
  {"key":"QD3YARXP","version":29,"data":{"key":"QD3YARXP","version":29,"itemType":"journalArticle","title":"Climate Forcing and Trends of Organic Aerosols in the Community Earth System Model (CESM2)","creators":[{"creatorType":"author","firstName":"S.","lastName":"Tilmes"},{"creatorType":"author","firstName":"A.","lastName":"Hodzic"},{"creatorType":"author","firstName":"L. K.","lastName":"Emmons"},{"creatorType":"author","firstName":"M. J.","lastName":"Mills"},{"creatorType":"author","firstName":"A.","lastName":"Gettelman"},{"creatorType":"author","firstName":"D. E.","lastName":"Kinnison"},{"creatorType":"author","firstName":"M.","lastName":"Park"},{"creatorType":"author","firstName":"J.‐F.","lastName":"Lamarque"},{"creatorType":"author","firstName":"F.","lastName":"Vitt"},{"creatorType":"author","firstName":"M.","lastName":"Shrivastava"},{"creatorType":"author","firstName":"P.","lastName":"Campuzano‐Jost"},{"creatorType":"author","firstName":"J. L.","lastName":"Jimenez"},{"creatorType":"author","firstName":"X.","lastName":"Liu"}],"abstractNote":"","publicationTitle":"Journal of Advances in Modeling Earth Systems","volume":"11","issue":"12","pages":"4323-4351","date":"12/2019","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"J. Adv. Model. Earth Syst.","language":"en","DOI":"10.1029/2019MS001827","ISSN":"1942-2466, 1942-2466","shortTitle":"","url":"https://onlinelibrary.wiley.com/doi/abs/10.1029/2019MS001827","accessDate":"2022-04-27T00:43:07Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","deleted":1,"tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T00:43:07Z","dateModified":"2022-04-27T00:43:07Z"}}


key: 5V97R9HP
data:
  {"key":"5V97R9HP","version":17,"data":{"key":"5V97R9HP","version":17,"itemType":"webpage","title":"Communicating with Slack","creators":[],"abstractNote":"","websiteTitle":"","websiteType":"","date":"","shortTitle":"","url":"https://geo-python-site.readthedocs.io/en/latest/lessons/L1/slack-usage.html","accessDate":"2022-04-27T00:32:52Z","language":"","rights":"","extra":"","deleted":1,"tags":[],"collections":[],"relations":{},"dateAdded":"2022-04-27T00:32:52Z","dateModified":"2022-04-27T00:32:52Z"}}


key: VWGSM6E6
data:
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key: HCAH4F98
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key: HQCVRKB5
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key: YSQEB39N
data:
  {"key":"YSQEB39N","version":653,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/YSQEB39N","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/YSQEB39N","type":"text/html"}},"meta":{"creatorSummary":"Xiang et al.","parsedDate":"2020","numChildren":0},"data":{"key":"YSQEB39N","version":653,"itemType":"journalArticle","title":"Numerical study of the physical and chemical effects of hydrogen addition on laminar premixed combustion characteristics of methane and ethane","creators":[{"creatorType":"author","firstName":"Longkai","lastName":"Xiang"},{"creatorType":"author","firstName":"Hantao","lastName":"Jiang"},{"creatorType":"author","firstName":"Fei","lastName":"Ren"},{"creatorType":"author","firstName":"Huaqiang","lastName":"Chu"},{"creatorType":"author","firstName":"Pan","lastName":"Wang"}],"abstractNote":"","publicationTitle":"International Journal of Hydrogen Energy","volume":"45","issue":"39","pages":"20501-20514","date":"08/2020","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"International Journal of Hydrogen Energy","language":"en","DOI":"10.1016/j.ijhydene.2019.11.040","ISSN":"03603199","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S0360319919342211","accessDate":"2022-08-20T19:38:28Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:38:28Z","dateModified":"2022-08-20T19:38:29Z"}}


key: 48W2F62A
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key: 8BHTWT43
data:
  {"key":"8BHTWT43","version":653,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/8BHTWT43","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/8BHTWT43","type":"text/html"}},"meta":{"creatorSummary":"Ahmad et al.","parsedDate":"2021","numChildren":0},"data":{"key":"8BHTWT43","version":653,"itemType":"journalArticle","title":"Effects of ethane addition on diesel-methane dual-fuel combustion in a heavy-duty engine","creators":[{"creatorType":"author","firstName":"Zeeshan","lastName":"Ahmad"},{"creatorType":"author","firstName":"Ossi","lastName":"Kaario"},{"creatorType":"author","firstName":"Shervin","lastName":"Karimkashi"},{"creatorType":"author","firstName":"Cheng","lastName":"Qiang"},{"creatorType":"author","firstName":"Ville","lastName":"Vuorinen"},{"creatorType":"author","firstName":"Martti","lastName":"Larmi"}],"abstractNote":"The present study is a continuation of the previous work by Ahmad et al. (2020), in which ethane (C2H6) enriched diesel-methane (CH4) dual-fuel (DF) combustion was experimentally investigated in a single-cylinder heavy-duty engine. Here, the experiments of ethane enriched DF combustion are carried out with new details together with supporting zero-dimensional (0D) and one-dimensional (1D) chemical kinetics simulations. Three port-fuel injected (PFI) gaseous blends of pure methane with varying ethane concentrations of 0%, 10%, and 20% are used as the main fuels. The PFI gaseous blend provides 97% of the total-fuel energy (TFE), which is ignited by a small 3% (TFE based) pilot diesel. Experiments are performed under lean condition (∅gas = 0.52) for two engine speeds while keeping the TFE and other operating conditions constant. Calculated results from 0D and 1D simulations under engine relevant conditions including theoretical combustion mode analysis (β-curve) are used to deepen the phenomenological understanding of the experimental results. The results reveal that adding ethane into pure methane has minor effects on the pilot-diesel ignition timing. However, ethane addition greatly en­ hances the ignitability of methane after the start of combustion. Ethane enriched gaseous blends yield higher thermal efficiency and reduce combustion duration compared to pure methane. According to combustion mode analysis, ethane tendency to promote spontaneous autoignition may be one of the reasons for improving overall combustion performance. It is observed that ethane enriched gaseous blends produce lower unburned methane (UB-CH4) and unburned hydrocarbons (THC) accompanied with higher nitrogen oxides (NOx) because of the higher combustion efficiency. Furthermore, ethane addition considerably helps to reduce cycle-to-cycle varia­ tions under lean conditions compared to pure methane.","publicationTitle":"Fuel","volume":"289","issue":"","pages":"119834","date":"04/2021","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Fuel","language":"en","DOI":"10.1016/j.fuel.2020.119834","ISSN":"00162361","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S0016236120328301","accessDate":"2022-08-20T19:38:38Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:38:38Z","dateModified":"2022-08-20T19:38:39Z"}}


key: J8KI9D7M
data:
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key: YDNTD2JK
data:
  {"key":"YDNTD2JK","version":653,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/YDNTD2JK","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/YDNTD2JK","type":"text/html"}},"meta":{"creatorSummary":"Macfarlane et al.","parsedDate":"2018","numChildren":0},"data":{"key":"YDNTD2JK","version":653,"itemType":"journalArticle","title":"The evolution of autoignition kernels in turbulent flames of dimethyl ether","creators":[{"creatorType":"author","firstName":"Andrew R.W.","lastName":"Macfarlane"},{"creatorType":"author","firstName":"Matthew","lastName":"Dunn"},{"creatorType":"author","firstName":"Mrinal","lastName":"Juddoo"},{"creatorType":"author","firstName":"Assaad","lastName":"Masri"}],"abstractNote":"","publicationTitle":"Combustion and Flame","volume":"197","issue":"","pages":"182-196","date":"11/2018","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Combustion and Flame","language":"en","DOI":"10.1016/j.combustflame.2018.07.022","ISSN":"00102180","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S0010218018303511","accessDate":"2022-08-20T19:39:09Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:39:10Z","dateModified":"2022-08-20T19:39:10Z"}}


key: L8MIPTQA
data:
  {"key":"L8MIPTQA","version":653,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/L8MIPTQA","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/L8MIPTQA","type":"text/html"},"up":{"href":"https://api.zotero.org/users/2422938/items/YDNTD2JK","type":"application/json"}},"meta":{"numChildren":0},"data":{"key":"L8MIPTQA","version":653,"parentItem":"YDNTD2JK","itemType":"attachment","linkMode":"imported_file","title":"Macfarlane et al. - 2018 - The evolution of autoignition kernels in turbulent.pdf","accessDate":"","url":"","note":"","contentType":"application/pdf","charset":"","filename":"Macfarlane et al. - 2018 - The evolution of autoignition kernels in turbulent.pdf","md5":null,"mtime":null,"tags":[],"relations":{},"dateAdded":"2022-08-20T19:37:47Z","dateModified":"2022-08-20T19:39:11Z"}}


key: IE393K6V
data:
  {"key":"IE393K6V","version":653,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/IE393K6V","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/IE393K6V","type":"text/html"}},"meta":{"creatorSummary":"Lawson et al.","parsedDate":"2021","numChildren":0},"data":{"key":"IE393K6V","version":653,"itemType":"journalArticle","title":"Autoignition of reacting mixtures at engine-relevant conditions using confined spherically expanding flames","creators":[{"creatorType":"author","firstName":"Robert","lastName":"Lawson"},{"creatorType":"author","firstName":"Vyaas","lastName":"Gururajan"},{"creatorType":"author","firstName":"Ashkan","lastName":"Movaghar"},{"creatorType":"author","firstName":"Fokion N.","lastName":"Egolfopoulos"}],"abstractNote":"Propagation of a confined spherically expanding flame induces isentropic compression that can culminate in autoignition and/or detonation under conducive thermodynamic conditions. This relatively simple technique measures a distinct ‘characteristic ignition delay time’ and complements other established approaches such as the rapid compression machine and shock tube. The present study details this methodology by examining the autoignition characteristics of dimethyl-ether/oxygen/nitrogen/helium reactive mixtures for equivalence ratios of 0.6 and 0.9, an initial temperature of 468 K, and initial pressures of 3 to 6 atm. The experimental results display the classic two-stage ignition typical of dimethyl-ether oxidation at low-temperatures with first-stage ignition occurring at approximately 3.6 times the initial pressure. To aid in the interpretation of the experimental results, two numerical models were used: a zero-dimensional batch reactor model, which accepts experimental pressure-time history and calculates the sensitivities of characteristic ignition delay times to kinetics, and a low Mach number, Lagrangian one-dimensional code that was developed to model both flame propagation and end-gas autoignition. Simulation results were shown to adequately capture the physics of unsteady flame propagation, end-gas autoignition, and the controlling reactions of the latter. It was found also that under certain conditions the behavior of first and second ignition stages could be modified by unsteady pressure effects.","publicationTitle":"Proceedings of the Combustion Institute","volume":"38","issue":"2","pages":"2285-2293","date":"2021","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Proceedings of the Combustion Institute","language":"en","DOI":"10.1016/j.proci.2020.06.224","ISSN":"15407489","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S1540748920303163","accessDate":"2022-08-20T19:40:20Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:40:20Z","dateModified":"2022-08-20T19:40:21Z"}}


key: RFYXHISJ
data:
  {"key":"RFYXHISJ","version":654,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/RFYXHISJ","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/RFYXHISJ","type":"text/html"}},"meta":{"creatorSummary":"Liu et al.","parsedDate":"2018","numChildren":0},"data":{"key":"RFYXHISJ","version":654,"itemType":"journalArticle","title":"A rapid compression machine study of autoignition, spark-ignition and flame propagation characteristics of H2/CH4/CO/air mixtures","creators":[{"creatorType":"author","firstName":"Changpeng","lastName":"Liu"},{"creatorType":"author","firstName":"Heping","lastName":"Song"},{"creatorType":"author","firstName":"Peng","lastName":"Zhang"},{"creatorType":"author","firstName":"Zhi","lastName":"Wang"},{"creatorType":"author","firstName":"Margaret S","lastName":"Wooldridge"},{"creatorType":"author","firstName":"Xin","lastName":"He"},{"creatorType":"author","firstName":"Guotao","lastName":"Suo"}],"abstractNote":"","publicationTitle":"Combustion and Flame","volume":"188","issue":"","pages":"150-161","date":"02/2018","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Combustion and Flame","language":"en","DOI":"10.1016/j.combustflame.2017.09.031","ISSN":"00102180","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S0010218017303681","accessDate":"2022-08-20T19:41:22Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:41:22Z","dateModified":"2022-08-20T19:41:22Z"}}


key: HNWJZGDN
data:
  {"key":"HNWJZGDN","version":654,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/HNWJZGDN","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/HNWJZGDN","type":"text/html"},"up":{"href":"https://api.zotero.org/users/2422938/items/RFYXHISJ","type":"application/json"},"enclosure":{"type":"application/pdf","href":"https://api.zotero.org/users/2422938/items/HNWJZGDN/file/view","title":"Liu et al. - 2018 - A rapid compression machine study of autoignition,.pdf","length":3150154}},"meta":{"numChildren":0},"data":{"key":"HNWJZGDN","version":654,"parentItem":"RFYXHISJ","itemType":"attachment","linkMode":"imported_file","title":"Liu et al. - 2018 - A rapid compression machine study of autoignition,.pdf","accessDate":"","url":"","note":"","contentType":"application/pdf","charset":"","filename":"Liu et al. - 2018 - A rapid compression machine study of autoignition,.pdf","md5":"c16c25801a1a7f421f524097d8776428","mtime":1661024483000,"tags":[],"relations":{},"dateAdded":"2022-08-20T19:37:52Z","dateModified":"2022-08-20T19:41:23Z"}}


key: MK33EJFZ
data:
  {"key":"MK33EJFZ","version":654,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/MK33EJFZ","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/MK33EJFZ","type":"text/html"}},"meta":{"creatorSummary":"Frolov et al.","parsedDate":"2013","numChildren":0},"data":{"key":"MK33EJFZ","version":654,"itemType":"journalArticle","title":"Numerical simulation of flame propagation and localized preflame autoignition in enclosures","creators":[{"creatorType":"author","firstName":"S.M.","lastName":"Frolov"},{"creatorType":"author","firstName":"V.S.","lastName":"Ivanov"},{"creatorType":"author","firstName":"B.","lastName":"Basara"},{"creatorType":"author","firstName":"M.","lastName":"Suffa"}],"abstractNote":"A novel computational approach based on the coupled 3D Flame-TrackingeParticle (FTP) method is used for numerical simulation of conﬁned explosions caused by preﬂame autoignition. The Flame-Tracking (FT) technique implies continuous tracing of the mean ﬂame surface and application of the laminar/ turbulent ﬂame velocity concepts. The Particle method is based on the joint velocityescalar probability density function approach for simulating reactive mixture autoignition in the preﬂame zone. The coupled algorithm is supplemented with the database of tabulated laminar ﬂame velocities as well as with reaction rates of hydrocarbon fuel oxidation in wide ranges of initial temperature, pressure, and equivalence ratio. The main advantage of the FTP method is that it covers both possible modes of premixed combustion, namely, frontal and volumetric. As examples, combustion of premixed hydrogeneair, propaneeair, and n-heptaneeair mixtures in enclosures of different geometry is considered. At certain conditions, volumetric hot spots ahead of the propagating ﬂame are identiﬁed. These hot spots transform to localized exothermic centers giving birth to spontaneous ignition waves traversing the preﬂame zone at very high apparent velocities, i.e., nearly homogeneous preﬂame explosion occurs. The abrupt pressure rise results in the formation of shock waves producing high overpressure peaks after reﬂections from enclosure walls.","publicationTitle":"Journal of Loss Prevention in the Process Industries","volume":"26","issue":"2","pages":"302-309","date":"3/2013","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Journal of Loss Prevention in the Process Industries","language":"en","DOI":"10.1016/j.jlp.2011.09.007","ISSN":"09504230","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S0950423011001665","accessDate":"2022-08-20T19:41:39Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:41:39Z","dateModified":"2022-08-20T19:41:39Z"}}


key: TB8LEYPK
data:
  {"key":"TB8LEYPK","version":654,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/TB8LEYPK","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/TB8LEYPK","type":"text/html"}},"meta":{"creatorSummary":"Yu et al.","parsedDate":"2017","numChildren":0},"data":{"key":"TB8LEYPK","version":654,"itemType":"journalArticle","title":"Effects of flame propagation speed and chamber size on end-gas autoignition","creators":[{"creatorType":"author","firstName":"Hao","lastName":"Yu"},{"creatorType":"author","firstName":"Chengken","lastName":"Qi"},{"creatorType":"author","firstName":"Zheng","lastName":"Chen"}],"abstractNote":"End-gas autoignition has direct relevance to engine knock and thereby has been extensively studied. However, in the literature there are still some contradictions on how different factors affect end-gas autoignition and knock intensity. Specifically, there is contradictory literature on (1) whether faster combustion may promote or inhibit end-gas autoignition and engine knock, and (2) whether knock intensity increases or decreases with burned mass fraction (BMF). To answer these two questions, one-dimensional flame propagation and end-gas autoignition in a closed cylindrical chamber are investigated and the effects of flame propagation speed and chamber size on end-gas autoignition are examined in this study. In the transient numerical simulation, two fuels, hydrogen and iso-octane, are studied; and detailed chemistry is considered. It is shown that if the flame propagation is fast enough or the chamber is small enough, end-gas autoignition and knock can be prevented; otherwise, the knock intensity may increase as the flame propagation speed increases or as the chamber size decreases. The maximum pressure is found to change non-monotonically with the BMF as well as the flame propagation speed and chamber size. This helps to explain why there is contradictory literature on those two questions mentioned above. The answers to these two questions depend on the amount of unburned mixture at the moment of end-gas autoignition: if there is enough unburned mixture before end-gas autoignition, the maximum pressure increases with the flame propagation speed and BMF; otherwise, the opposite trend occurs. Besides, comparison between the results for hydrogen and iso-octane indicates that end-gas chemical reaction and heat release occurring before autoignition can greatly reduce the maximum pressure.","publicationTitle":"Proceedings of the Combustion Institute","volume":"36","issue":"3","pages":"3533-3541","date":"2017","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Proceedings of the Combustion Institute","language":"en","DOI":"10.1016/j.proci.2016.07.123","ISSN":"15407489","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S1540748916303819","accessDate":"2022-08-20T19:41:52Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:41:52Z","dateModified":"2022-08-20T19:41:52Z"}}


key: IKEJM85N
data:
  {"key":"IKEJM85N","version":654,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/IKEJM85N","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/IKEJM85N","type":"text/html"}},"meta":{"creatorSummary":"Zhang and Ju","parsedDate":"2020","numChildren":0},"data":{"key":"IKEJM85N","version":654,"itemType":"journalArticle","title":"Structures and propagation speeds of autoignition-assisted premixed n-heptane/air cool and warm flames at elevated temperatures and pressures","creators":[{"creatorType":"author","firstName":"Tianhan","lastName":"Zhang"},{"creatorType":"author","firstName":"Yiguang","lastName":"Ju"}],"abstractNote":"","publicationTitle":"Combustion and Flame","volume":"211","issue":"","pages":"8-17","date":"01/2020","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Combustion and Flame","language":"en","DOI":"10.1016/j.combustflame.2019.09.019","ISSN":"00102180","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S001021801930433X","accessDate":"2022-08-20T19:41:57Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:41:57Z","dateModified":"2022-08-20T19:41:58Z"}}


key: SI8C3IS9
data:
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key: W3ILNZLQ
data:
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key: UJPYR9BA
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key: 39BAL495
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key: RL3DZRYF
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key: F3ASDX5Y
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key: RW7NJN3K
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key: RRCM6YNC
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key: 46HFXRKT
data:
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key: 42MJRGLG
data:
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key: 62FAMBWM
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key: A6BUFB7P
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key: KASEK8JE
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key: XI7SFXSG
data:
  {"key":"XI7SFXSG","version":663,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/XI7SFXSG","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/XI7SFXSG","type":"text/html"}},"meta":{"creatorSummary":"Qadiri and AlFantazi","parsedDate":"2022","numChildren":0},"data":{"key":"XI7SFXSG","version":663,"itemType":"journalArticle","title":"Numerical 1-D simulations on Single-Cylinder stationary spark ignition engine using Micro-Emulsions, gasoline, and hydrogen in dual fuel mode","creators":[{"creatorType":"author","firstName":"Ufaith","lastName":"Qadiri"},{"creatorType":"author","firstName":"Akram","lastName":"AlFantazi"}],"abstractNote":"","publicationTitle":"Cleaner Chemical Engineering","volume":"2","issue":"","pages":"100009","date":"06/2022","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Cleaner Chemical Engineering","language":"en","DOI":"10.1016/j.clce.2022.100009","ISSN":"27727823","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S2772782322000092","accessDate":"2022-08-20T19:43:19Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:43:19Z","dateModified":"2022-08-20T19:43:20Z"}}


key: Y7VEHGDX
data:
  {"key":"Y7VEHGDX","version":663,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/Y7VEHGDX","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/Y7VEHGDX","type":"text/html"},"up":{"href":"https://api.zotero.org/users/2422938/items/XI7SFXSG","type":"application/json"}},"meta":{"numChildren":0},"data":{"key":"Y7VEHGDX","version":663,"parentItem":"XI7SFXSG","itemType":"attachment","linkMode":"imported_file","title":"Qadiri and AlFantazi - 2022 - Numerical 1-D simulations on Single-Cylinder stati.pdf","accessDate":"","url":"","note":"","contentType":"application/pdf","charset":"","filename":"Qadiri and AlFantazi - 2022 - Numerical 1-D simulations on Single-Cylinder stati.pdf","md5":null,"mtime":null,"tags":[],"relations":{},"dateAdded":"2022-08-20T19:38:11Z","dateModified":"2022-08-20T19:43:21Z"}}


key: 52CK3TL2
data:
  {"key":"52CK3TL2","version":663,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/52CK3TL2","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/52CK3TL2","type":"text/html"}},"meta":{"creatorSummary":"Karimkashi et al.","parsedDate":"2022","numChildren":0},"data":{"key":"52CK3TL2","version":663,"itemType":"journalArticle","title":"Effects of hydrogen enrichment and turbulence intensity on the combustion mode in locally stratified dual-fuel mixtures of n-dodecane/methane","creators":[{"creatorType":"author","firstName":"Shervin","lastName":"Karimkashi"},{"creatorType":"author","firstName":"Ossi","lastName":"Kaario"},{"creatorType":"author","firstName":"Ville","lastName":"Vuorinen"}],"abstractNote":"In dual-fuel (DF) engines, a high-reactivity fuel (HRF) ignites a low-reactivity fuel (LRF) premixed with air. Identification of the combustion mode after autoignition in DF engines with different fuel combinations and under various mixture stratification levels is of crucial importance since the combustion mode may affect the engine performance and emissions levels. However, to avoid expensive computational or experimental tests for different fuel combinations under various initial conditions, an analytical diagnostics tool can help identify the modes of combustion. Recently, we developed an a-priori tool (𝛽-curve), which separates between the deflagration and spontaneous combustion modes in transient problems based on two parameters: HRF stratification amplitude and wavelength. However, the developed analysis was only evaluated for a single fuel combination and under 2D turbulent conditions. The present study extends our previous work by (1) evaluating the 1D 𝛽-curve analysis for more common fuel combinations including hydrogen, and (2) extending the combustion mode analysis to 3D turbulent combustion. First, using 1D numerical simulations, the combustion mode for a new DF combination of n-dodecane (HRF) and methane (LRF) with and without hydrogen enrichment in the LRF blend is investigated. Although hydrogen enrichment shortens the combustion duration, its role in changing the combustion mode remains subtle. Therefore, only n-dodecane/methane (no hydrogen enrichment) is considered in the 3D simulations to avoid highly expensive 3D numerical simulations with hydrogen enrichment. Second, using flame-resolved 3D numerical simulations, variations of the combustion mode for DF n-dodecane/methane mixtures at three different turbulence intensities are studied. It is observed that high turbulence levels can switch the combustion mode from deflagration to autoignition. For the first time, the diagnostic tool is evaluated compared to 3D turbulent numerical simulations and a correction factor is proposed in the 𝛽-curve equation.","publicationTitle":"Applications in Energy and Combustion Science","volume":"10","issue":"","pages":"100072","date":"06/2022","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Applications in Energy and Combustion Science","language":"en","DOI":"10.1016/j.jaecs.2022.100072","ISSN":"2666352X","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S2666352X22000164","accessDate":"2022-08-20T19:43:25Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["YNSLQKNA"],"relations":{},"dateAdded":"2022-08-20T19:43:25Z","dateModified":"2022-08-20T19:43:26Z"}}


key: JEAHLU6U
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key: X8S5VA7T
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key: VHMW2AUL
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key: ZQ6BVFJE
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key: 28LFNFQI
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  {"key":"28LFNFQI","version":692,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/28LFNFQI","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/28LFNFQI","type":"text/html"},"up":{"href":"https://api.zotero.org/users/2422938/items/9SB6QJFW","type":"application/json"}},"meta":{},"data":{"key":"28LFNFQI","version":692,"parentItem":"9SB6QJFW","itemType":"annotation","annotationType":"highlight","annotationText":"For all simulation cases, the reaction front began as a deflagration.","annotationComment":"","annotationColor":"#ffd400","annotationPageLabel":"2085","annotationSortIndex":"00008|002183|00559","annotationPosition":"{\"pageIndex\":8,\"rects\":[[174.667,226.572,293.572,234.535],[42.52,216.084,197.881,224.047]]}","tags":[],"relations":{},"dateAdded":"2022-08-20T23:46:03Z","dateModified":"2022-08-20T23:46:03Z"}}


key: N6JRZ4HY
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key: VME77KKQ
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key: UXH957NK
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key: 3ULBJ3TS
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key: MSZT3SX7
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key: J9SXTZBH
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key: ACI5KRQW
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key: RIN4JTDZ
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key: 5YXM2NCI
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key: ZFKNRRP5
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key: VBHGUTJZ
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key: U8XZVX45
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key: 32CNM3M6
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key: 2D4DK54J
data:
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key: IMAL9RWV
data:
  {"key":"IMAL9RWV","version":765,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/IMAL9RWV","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/IMAL9RWV","type":"text/html"},"up":{"href":"https://api.zotero.org/users/2422938/items/TCT4743U","type":"application/json"}},"meta":{},"data":{"key":"IMAL9RWV","version":765,"parentItem":"TCT4743U","itemType":"annotation","annotationType":"highlight","annotationText":"In the post-flame section, the combustion process gradually reached completion.","annotationComment":"","annotationColor":"#ff6666","annotationPageLabel":"520","annotationSortIndex":"00007|001590|00643","annotationPosition":"{\"pageIndex\":7,\"rects\":[[94.41,142.024,288.874,150.122],[37.605,131.566,150.514,139.664]]}","tags":[],"relations":{},"dateAdded":"2022-08-21T00:31:01Z","dateModified":"2022-08-21T00:31:01Z"}}


key: F3Q32LJ6
data:
  {"key":"F3Q32LJ6","version":766,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/F3Q32LJ6","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/F3Q32LJ6","type":"text/html"},"up":{"href":"https://api.zotero.org/users/2422938/items/TCT4743U","type":"application/json"}},"meta":{},"data":{"key":"F3Q32LJ6","version":766,"parentItem":"TCT4743U","itemType":"annotation","annotationType":"highlight","annotationText":"the propagation speed of a flame under autoignitive conditions was affected by the accumulation of preflame reactions, which was related to the spatial location of the flame front. Under certain conditions (e.g., τ f / τ ig = 0.2–0.6), the flame speed showed a linear correlation with the pre-flame length.","annotationComment":"","annotationColor":"#ff6666","annotationPageLabel":"520","annotationSortIndex":"00007|001734|00675","annotationPosition":"{\"pageIndex\":7,\"rects\":[[127.537,110.641,288.892,118.739],[37.605,100.183,288.875,108.281],[37.605,89.716,288.915,97.814],[37.605,77.795,288.899,88.137],[37.605,68.8,288.904,76.898]]}","tags":[],"relations":{},"dateAdded":"2022-08-21T00:31:44Z","dateModified":"2022-08-21T00:31:44Z"}}


key: CYXMRLDZ
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key: GR2PFFLR
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key: GZZBMYKM
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  {"key":"GZZBMYKM","version":795,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/GZZBMYKM","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/GZZBMYKM","type":"text/html"},"up":{"href":"https://api.zotero.org/users/2422938/items/62FAMBWM","type":"application/json"}},"meta":{},"data":{"key":"GZZBMYKM","version":795,"parentItem":"62FAMBWM","itemType":"annotation","annotationType":"highlight","annotationText":"detailed chemical kinetics performed using CONVERGETM.","annotationComment":"","annotationColor":"#ffd400","annotationPageLabel":"11","annotationSortIndex":"00010|004719|00324","annotationPosition":"{\"pageIndex\":10,\"rects\":[[467.886,461.326,557.8,469.424],[306.597,450.868,437.485,460.257]]}","tags":[],"relations":{},"dateAdded":"2022-08-21T16:23:32Z","dateModified":"2022-08-21T16:23:32Z"}}


key: YWSS4QF6
data:
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key: MADRU4BR
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key: B4WDXJNX
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key: SIEIL8C3
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key: X3PTNQCI
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key: KI9MLCDT
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key: QTYA4QPZ
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key: GRA5IXBY
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key: VUQKJ7FJ
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key: BT972P3A
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key: NI68BG6E
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key: YRXMR2JD
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key: 96NWKU7N
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key: RMLH4VEW
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key: TSDDYGDQ
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key: U7GKV7NR
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key: AZHZUV6X
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key: PSJCRH5C
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key: UG9G7AKA
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key: 8NM9QPVW
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key: Z9JIE8GG
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key: W6963YMN
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key: B7WWQMZW
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key: RNWS35T8
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key: BXV22K95
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key: VE23L2HP
data:
  {"key":"VE23L2HP","version":935,"library":{"type":"user","id":2422938,"name":"aps121","links":{"alternate":{"href":"https://www.zotero.org/aps121","type":"text/html"}}},"links":{"self":{"href":"https://api.zotero.org/users/2422938/items/VE23L2HP","type":"application/json"},"alternate":{"href":"https://www.zotero.org/aps121/items/VE23L2HP","type":"text/html"}},"meta":{"creatorSummary":"Oevermann et al.","parsedDate":"2008","numChildren":0},"data":{"key":"VE23L2HP","version":935,"itemType":"journalArticle","title":"Investigation of autoignition under thermal stratification using linear eddy modeling","creators":[{"creatorType":"author","firstName":"M.","lastName":"Oevermann"},{"creatorType":"author","firstName":"H.","lastName":"Schmidt"},{"creatorType":"author","firstName":"A.R.","lastName":"Kerstein"}],"abstractNote":"The inﬂuence of thermal stratiﬁcation on autoignition at constant volume and high pressure is investigated under turbulent conditions using the one-dimensional linear eddy model (LEM) and detailed hydrogen/air chemistry. Results are presented for the inﬂuence of initial temperature inhomogeneities on the heat release rate and the relative importance of diffusion and chemical reactions. The predicted heat release rates are compared with heat release rates of recent published studies obtained by two-dimensional direct numerical simulations (DNS). Using the deﬁnition of Chen et al. [Combust. Flame 145 (2006) 145–159] for the displacement speed of the H2 mass fraction tracked at the location of maximum heat release, and a comparison of budget terms, different combustion modes including ignition-front propagation and deﬂagration waves are identiﬁed and the results are compared to the DNS data. The LEM approach shows qualitatively and quantitatively reasonable agreement with the DNS data over the whole range of investigated temperature ﬂuctuations. The results presented in this work suggest that LEM is a potential candidate as a submodel for CFD calculations of HCCI engines.","publicationTitle":"Combustion and Flame","volume":"155","issue":"3","pages":"370-379","date":"11/2008","series":"","seriesTitle":"","seriesText":"","journalAbbreviation":"Combustion and Flame","language":"en","DOI":"10.1016/j.combustflame.2008.04.020","ISSN":"00102180","shortTitle":"","url":"https://linkinghub.elsevier.com/retrieve/pii/S0010218008001338","accessDate":"2022-08-21T23:29:45Z","archive":"","archiveLocation":"","libraryCatalog":"DOI.org (Crossref)","callNumber":"","rights":"","extra":"","tags":[],"collections":["BW43546C"],"relations":{},"dateAdded":"2022-08-21T23:29:45Z","dateModified":"2022-08-21T23:29:46Z"}}


key: WVILWMI7
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key: 9DYT8EWT
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key: PGTSML9N
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key: UBLN8V8P
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key: PAT53LCP
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key: UHI24AFG
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key: MBKSYHLL
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key: E7E2U4VS
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key: CIAXC85I
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key: RCTLCQDV
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key: US3IE2V5
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key: QSSMIGNE
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key: YYKXM3XV
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key: XMPBBPUH
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key: X89LW9SF
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key: 4IDGN4VA
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key: RXZZPAZF
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key: PLWVG3RZ
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key: KMZNJ85E
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key: 4DWNCCS3
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key: HF2TEVHD
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key: PNDGY5QQ
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key: 5PJ6MZ47
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