{"data":{"id":"10.6084/m9.figshare.1446157","type":"dois","attributes":{"doi":"10.6084/m9.figshare.1446157","prefix":"10.6084","suffix":"m9.figshare.1446157","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Lamige, Sylvain","nameType":"Personal","givenName":"Sylvain","familyName":"Lamige","affiliation":[],"nameIdentifiers":[]},{"name":"Lyons, Kevin M.","nameType":"Personal","givenName":"Kevin M.","familyName":"Lyons","affiliation":[],"nameIdentifiers":[]},{"name":"Galizzi, Cédric","nameType":"Personal","givenName":"Cédric","familyName":"Galizzi","affiliation":[],"nameIdentifiers":[]},{"name":"Kühni, Manuel","nameType":"Personal","givenName":"Manuel","familyName":"Kühni","affiliation":[],"nameIdentifiers":[]},{"name":"Éric Mathieu","affiliation":[],"nameIdentifiers":[]},{"name":"Escudié, Dany","nameType":"Personal","givenName":"Dany","familyName":"Escudié","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Lifting and Splitting of Nonpremixed Methane/Air Flames Due to Reactant Preheating"}],"publisher":"Taylor \u0026 Francis","container":{},"publicationYear":2015,"subjects":[{"subject":"Computational Biology"},{"subject":"Plant Biology"},{"subject":"FOS: Biological sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Biological sciences","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"110309 Infectious Diseases","subjectScheme":"FOR"},{"subject":"FOS: Health sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Health sciences","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Biological Sciences"},{"subject":"Ecology"},{"subject":"Earth and Environmental Sciences"},{"subject":"Evolutionary Biology"},{"subject":"Physiology"},{"subject":"Microbiology"},{"subject":"Biophysics"}],"contributors":[],"dates":[{"date":"2015-06-11","dateType":"Created"},{"date":"2015-12-03","dateType":"Updated"},{"date":"2015","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1080/00102202.2015.1059829","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["485 Bytes"],"formats":[],"version":null,"rightsList":[{"rights":"Creative Commons Attribution 4.0 International","rightsUri":"https://creativecommons.org/licenses/by/4.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc-by-4.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"In order to assess the impact of initial reactant temperature on the occurrence of local extinction (LE) and the subsequent lifting process of non-premixed attached flames with increasing fuel injection velocity, hydroxyl radical planar laser-induced fluorescence (OH-PLIF) and high-speed CH*-chemiluminescence visualizations were conducted in a methane/air jet-flame, with preheating up to 1000 K. LE occurrence probability increases when approaching lifting, and the preheating level (T\u003csub\u003eox,ref\u003c/sub\u003e) affects the probability density function (PDF) shape of LE axial origin. At low T\u003csub\u003eox,ref\u003c/sub\u003e, partial lifting events occur near the burner lip, eventually leading the flame to lift directly from the very flame base. At higher T\u003csub\u003eox,ref\u003c/sub\u003e, partial lifting events no longer occur, and LE is mostly witnessed in the flame breakpoint zone (axially from 1 to 3 jet diameters), resulting in a breakpoint lifting process. For very high T\u003csub\u003eox,ref\u003c/sub\u003e (1000 K), local extinctions become widespread in the breakpoint zone so that a stable split flame is achieved prior to the lifted regime.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"PD94bWwgdmVyc2lvbj0iMS4wIiBlbmNvZGluZz0iVVRGLTgiPz4KPHJlc291cmNlIHhtbG5zPSJodHRwOi8vZGF0YWNpdGUub3JnL3NjaGVtYS9rZXJuZWwtNCIgeG1sbnM6eHNpPSJodHRwOi8vd3d3LnczLm9yZy8yMDAxL1hNTFNjaGVtYS1pbnN0YW5jZSIgeHNpOnNjaGVtYUxvY2F0aW9uPSJodHRwOi8vZGF0YWNpdGUub3JnL3NjaGVtYS9rZXJuZWwtNCBodHRwOi8vc2NoZW1hLmRhdGFjaXRlLm9yZy9tZXRhL2tlcm5lbC00LjEvbWV0YWRhdGEueHNkIj4KICA8aWRlbnRpZmllciBpZGVudGlmaWVyVHlwZT0iRE9JIj4xMC42MDg0L005LkZJR1NIQVJFLjE0NDYxNTc8L2lkZW50aWZpZXI+CiAgPGNyZWF0b3JzPgogICAgPGNyZWF0b3I+CiAgICAgIDxjcmVhdG9yTmFtZT5TeWx2YWluIExhbWlnZTwvY3JlYXRvck5hbWU+CiAgICA8L2NyZWF0b3I+CiAgICA8Y3JlYXRvcj4KICAgICAgPGNyZWF0b3JOYW1lPktldmluIE0uIEx5b25zPC9jcmVhdG9yTmFtZT4KICAgIDwvY3JlYXRvcj4KICAgIDxjcmVhdG9yPgogICAgICA8Y3JlYXRvck5hbWU+Q8OpZHJpYyBHYWxpenppPC9jcmVhdG9yTmFtZT4KICAgIDwvY3JlYXRvcj4KICAgIDxjcmVhdG9yPgogICAgICA8Y3JlYXRvck5hbWU+TWFudWVsIEvDvGhuaTwvY3JlYXRvck5hbWU+CiAgICA8L2NyZWF0b3I+CiAgICA8Y3JlYXRvcj4KICAgICAgPGNyZWF0b3JOYW1lPsOJcmljIE1hdGhpZXU8L2NyZWF0b3JOYW1lPgogICAgPC9jcmVhdG9yPgogICAgPGNyZWF0b3I+CiAgICAgIDxjcmVhdG9yTmFtZT5EYW55IEVzY3VkacOpPC9jcmVhdG9yTmFtZT4KICAgIDwvY3JlYXRvcj4KICA8L2NyZWF0b3JzPgogIDx0aXRsZXM+CiAgICA8dGl0bGU+TGlmdGluZyBhbmQgU3BsaXR0aW5nIG9mIE5vbnByZW1peGVkIE1ldGhhbmUvQWlyIEZsYW1lcyBEdWUgdG8gUmVhY3RhbnQgUHJlaGVhdGluZzwvdGl0bGU+CiAgPC90aXRsZXM+CiAgPGRlc2NyaXB0aW9ucz4KICAgIDxkZXNjcmlwdGlvbiBkZXNjcmlwdGlvblR5cGU9IkFic3RyYWN0Ij4mbHQ7ZGl2Jmd0OyZsdDtwJmd0O0luIG9yZGVyIHRvIGFzc2VzcyB0aGUgaW1wYWN0IG9mIGluaXRpYWwgcmVhY3RhbnQgdGVtcGVyYXR1cmUgb24gdGhlIG9jY3VycmVuY2Ugb2YgbG9jYWwgZXh0aW5jdGlvbiAoTEUpIGFuZCB0aGUgc3Vic2VxdWVudCBsaWZ0aW5nIHByb2Nlc3Mgb2Ygbm9uLXByZW1peGVkIGF0dGFjaGVkIGZsYW1lcyB3aXRoIGluY3JlYXNpbmcgZnVlbCBpbmplY3Rpb24gdmVsb2NpdHksIGh5ZHJveHlsIHJhZGljYWwgcGxhbmFyIGxhc2VyLWluZHVjZWQgZmx1b3Jlc2NlbmNlIChPSC1QTElGKSBhbmQgaGlnaC1zcGVlZCBDSCotY2hlbWlsdW1pbmVzY2VuY2UgdmlzdWFsaXphdGlvbnMgd2VyZSBjb25kdWN0ZWQgaW4gYSBtZXRoYW5lL2FpciBqZXQtZmxhbWUsIHdpdGggcHJlaGVhdGluZyB1cCB0byAxMDAwIEsuIExFIG9jY3VycmVuY2UgcHJvYmFiaWxpdHkgaW5jcmVhc2VzIHdoZW4gYXBwcm9hY2hpbmcgbGlmdGluZywgYW5kIHRoZSBwcmVoZWF0aW5nIGxldmVsIChUJmx0O3N1YiZndDtveCxyZWYmbHQ7L3N1YiZndDspIGFmZmVjdHMgdGhlIHByb2JhYmlsaXR5IGRlbnNpdHkgZnVuY3Rpb24gKFBERikgc2hhcGUgb2YgTEUgYXhpYWwgb3JpZ2luLiBBdCBsb3cgVCZsdDtzdWImZ3Q7b3gscmVmJmx0Oy9zdWImZ3Q7LCBwYXJ0aWFsIGxpZnRpbmcgZXZlbnRzIG9jY3VyIG5lYXIgdGhlIGJ1cm5lciBsaXAsIGV2ZW50dWFsbHkgbGVhZGluZyB0aGUgZmxhbWUgdG8gbGlmdCBkaXJlY3RseSBmcm9tIHRoZSB2ZXJ5IGZsYW1lIGJhc2UuIEF0IGhpZ2hlciBUJmx0O3N1YiZndDtveCxyZWYmbHQ7L3N1YiZndDssIHBhcnRpYWwgbGlmdGluZyBldmVudHMgbm8gbG9uZ2VyIG9jY3VyLCBhbmQgTEUgaXMgbW9zdGx5IHdpdG5lc3NlZCBpbiB0aGUgZmxhbWUgYnJlYWtwb2ludCB6b25lIChheGlhbGx5IGZyb20gMSB0byAzIGpldCBkaWFtZXRlcnMpLCByZXN1bHRpbmcgaW4gYSBicmVha3BvaW50IGxpZnRpbmcgcHJvY2Vzcy4gRm9yIHZlcnkgaGlnaCBUJmx0O3N1YiZndDtveCxyZWYmbHQ7L3N1YiZndDsgKDEwMDAgSyksIGxvY2FsIGV4dGluY3Rpb25zIGJlY29tZSB3aWRlc3ByZWFkIGluIHRoZSBicmVha3BvaW50IHpvbmUgc28gdGhhdCBhIHN0YWJsZSBzcGxpdCBmbGFtZSBpcyBhY2hpZXZlZCBwcmlvciB0byB0aGUgbGlmdGVkIHJlZ2ltZS4mbHQ7L3AmZ3Q7Jmx0Oy9kaXYmZ3Q7PC9kZXNjcmlwdGlvbj4KICA8L2Rlc2NyaXB0aW9ucz4KICA8c3ViamVjdHM+CiAgICA8c3ViamVjdD5Db21wdXRhdGlvbmFsICBCaW9sb2d5PC9zdWJqZWN0PgogICAgPHN1YmplY3Q+UGxhbnQgQmlvbG9neTwvc3ViamVjdD4KICAgIDxzdWJqZWN0IHNjaGVtZVVSST0iaHR0cDovL3d3dy5hYnMuZ292LmF1L2F1c3N0YXRzL2Fic0AubnNmLzAvNkJCNDI3QUI5Njk2QzIyNUNBMjU3NDE4MDAwNDQ2M0UiIHN1YmplY3RTY2hlbWU9IkZPUiI+MTEwMzA5IEluZmVjdGlvdXMgRGlzZWFzZXM8L3N1YmplY3Q+CiAgICA8c3ViamVjdD5CaW9sb2dpY2FsIFNjaWVuY2VzPC9zdWJqZWN0PgogICAgPHN1YmplY3Q+RWNvbG9neTwvc3ViamVjdD4KICAgIDxzdWJqZWN0PkVhcnRoIGFuZCBFbnZpcm9ubWVudGFsIFNjaWVuY2VzPC9zdWJqZWN0PgogICAgPHN1YmplY3Q+RXZvbHV0aW9uYXJ5IEJpb2xvZ3k8L3N1YmplY3Q+CiAgICA8c3ViamVjdD5QaHlzaW9sb2d5PC9zdWJqZWN0PgogICAgPHN1YmplY3Q+TWljcm9iaW9sb2d5PC9zdWJqZWN0PgogICAgPHN1YmplY3Q+QmlvcGh5c2ljczwvc3ViamVjdD4KICA8L3N1YmplY3RzPgogIDxwdWJsaXNoZXI+VGF5bG9yICZhbXA7IEZyYW5jaXM8L3B1Ymxpc2hlcj4KICA8cHVibGljYXRpb25ZZWFyPjIwMTU8L3B1YmxpY2F0aW9uWWVhcj4KICA8ZGF0ZXM+CiAgICA8ZGF0ZSBkYXRlVHlwZT0iQ3JlYXRlZCI+MjAxNS0wNi0xMTwvZGF0ZT4KICAgIDxkYXRlIGRhdGVUeXBlPSJVcGRhdGVkIj4yMDE1LTEyLTAzPC9kYXRlPgogIDwvZGF0ZXM+CiAgPHJlc291cmNlVHlwZSByZXNvdXJjZVR5cGVHZW5lcmFsPSJEYXRhc2V0Ij5EYXRhc2V0PC9yZXNvdXJjZVR5cGU+CiAgPHNpemVzPgogICAgPHNpemU+NDg1IEJ5dGVzPC9zaXplPgogIDwvc2l6ZXM+CiAgPHJlbGF0ZWRJZGVudGlmaWVycz4KICAgIDxyZWxhdGVkSWRlbnRpZmllciByZWxhdGVkSWRlbnRpZmllclR5cGU9IkRPSSIgcmVsYXRpb25UeXBlPSJJc1N1cHBsZW1lbnRUbyI+MTAuMTA4MC8wMDEwMjIwMi4yMDE1LjEwNTk4Mjk8L3JlbGF0ZWRJZGVudGlmaWVyPgogIDwvcmVsYXRlZElkZW50aWZpZXJzPgogIDxyaWdodHNMaXN0PgogICAgPHJpZ2h0cyByaWdodHNVUkk9Imh0dHBzOi8vY3JlYXRpdmVjb21tb25zLm9yZy9saWNlbnNlcy9ieS80LjAvIj5DQyBCWSA0LjA8L3JpZ2h0cz4KICA8L3JpZ2h0c0xpc3Q+CjwvcmVzb3VyY2U+","url":"https://tandf.figshare.com/articles/dataset/Lifting_and_Splitting_of_Nonpremixed_Methane_Air_Flames_Due_to_Reactant_Preheating/1446157","contentUrl":null,"metadataVersion":3,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOv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