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dc.contributor.authorÆsøy, Eirik
dc.contributor.authorAguilar, Jose
dc.contributor.authorBothien, Mirko R.
dc.contributor.authorWorth, Nicholas
dc.contributor.authorDawson, James
dc.date.accessioned2021-11-03T07:21:54Z
dc.date.available2021-11-03T07:21:54Z
dc.date.created2021-08-11T18:09:58Z
dc.date.issued2021
dc.identifier.citationJournal of Engineering For Gas Turbines and Power. 2021, .en_US
dc.identifier.issn0742-4795
dc.identifier.urihttps://hdl.handle.net/11250/2827398
dc.description.abstractWe investigate the occurrence and source of modulations in the gain and phase of flame transfer functions (FTF) measured in perfectly premixed, bluff body stabilized CH4=H2 and pure H2 flames. The modulations are shown to be caused by flow disturbances originating from the upstream geometry, in particular the grub screws used to center the bluff body, indicative of a more generalized phenomenon of convective wave propagation. Velocity measurements are performed at various locations around the injector dump plane, inside the injector pipe, and in the wake of the bluff body to provide detailed insight into the flow. Peaks corresponding to natural shedding frequencies of the grub screws appear in the unforced velocity spectra and it is found that the magnitude of these convective modes depends on their location. Flame imaging and PIV measurements show that these disturbances do not show up in the mean velocity and flame shape which appear approximately axisymmetric. However, the urms and vrms fields capture a strong asymmetry due to convective disturbances. To further quantify the role of these convective disturbances, hydrodynamic transfer functions are constructed from the forced cold flow, and similar modulations observed in the FTFs are found. A strong correlation is obtained between the two transfer functions, subsequently, the modulations are shown to be centered on the vortex shedding frequency corresponding to the first convective mode. The reason behind the excitation of the first mode is due to a condition that states that for acoustic-convective interaction to be possible, the shedding (convective) frequency needs to be lower than the cutoff frequency of the flame response. This condition is shown to be more relevant for hydrogen flames compared to methane flames due to their shorter flame lengths and thus increased cutoff frequency. [DOI: 10.1115/1.4051960]en_US
dc.language.isoengen_US
dc.publisherASMEen_US
dc.titleAcoustic-Convective Interference in Transfer Functions of Methane/Hydrogen and Pure Hydrogen Flamesen_US
dc.typePeer revieweden_US
dc.typeJournal articleen_US
dc.description.versionacceptedVersionen_US
dc.rights.holderThis article will not be available due to copyright restrictions by ASMEen_US
dc.source.pagenumber13en_US
dc.source.journalJournal of Engineering For Gas Turbines and Poweren_US
dc.identifier.doi10.1115/1.4051960
dc.identifier.cristin1925423
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.fulltextpostprint
cristin.qualitycode1


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