Exploring the mechanisms leading to diffuse and filamentary modes in dielectric barrier discharges in N 2 with N 2 O admixtures

dc.bibliographicCitation.articleNumber35
dc.bibliographicCitation.firstPage35
dc.bibliographicCitation.issue3
dc.bibliographicCitation.journalTitleThe European Physical Journal D
dc.bibliographicCitation.volume77
dc.contributor.authorHöft, Hans
dc.contributor.authorBecker, Markus M.
dc.contributor.authorKettlitz, Manfred
dc.contributor.authorDap, Simon
dc.contributor.authorNaudé, Nicolas
dc.contributor.authorBrandenburg, Ronny
dc.contributor.authorWeltmann, Klaus-Dieter
dc.date.accessioned2025-02-26T09:42:03Z
dc.date.available2025-02-26T09:42:03Z
dc.date.issued2023
dc.description.abstractAbstract: The effects of nitrous oxide (N2O) in nitrogen (N2) on the development and morphology of sine-driven dielectric barrier discharges in a single-filament arrangement were studied. Detailed insight in the characteristics of the discharge and its development were obtained from electrical measurements combined with ICCD and streak camera recordings as well as numerical modelling. A miniaturised atmospheric pressure Townsend discharge (APTD) could be generated for admixtures up to 5 vol% N2O in N2 although N2O is an efficient collisional quencher of metastable nitrogen molecules. Increasing the high voltage amplitude led to a transition into a hybrid mode with the generation of an intermediate filament in addition to the diffuse, non-constricted APTD. A time-dependent, spatially one-dimensional fluid model was applied in order to study the underlying mechanisms causing the diffuse discharge characteristics. It was found that even for small N2O admixtures, the associative ionisation of atomic nitrogen and oxygen (O + N(2P) → NO+ + e) is the major electron source sustaining the volume memory effect and is therefore the reason for the formation of a diffuse APTD. Graphical abstract: [Figure not available: see fulltext.].eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/18596
dc.identifier.urihttps://doi.org/10.34657/17615
dc.language.isoeng
dc.publisherBerlin ; Heidelberg : Springer
dc.relation.doihttps://doi.org/10.1140/epjd/s10053-023-00601-z
dc.relation.essn1434-6079
dc.relation.issn1434-6060
dc.rights.licenseCC BY 4.0 Unported
dc.rights.urihttps://creativecommons.org/licenses/by/4.0
dc.subject.ddc530
dc.subject.otherDielectric barrier dischargeeng
dc.subject.otherDielectric deviceseng
dc.subject.otherDielectric materialseng
dc.subject.otherNitrogeneng
dc.subject.otherNitrogen oxideseng
dc.subject.otherAdmixtureeng
dc.subject.otherCollisionaleng
dc.subject.otherDielectric barrier dischargeseng
dc.subject.otherDiffuse modeeng
dc.subject.otherElectrical measurementeng
dc.subject.otherFilament arrangementeng
dc.subject.otherFilamentary modeeng
dc.subject.otherNitrous oxideeng
dc.subject.otherSingle filamentseng
dc.subject.otherTownsend dischargeseng
dc.subject.otherAtmospheric pressureeng
dc.titleExploring the mechanisms leading to diffuse and filamentary modes in dielectric barrier discharges in N 2 with N 2 O admixtureseng
dc.typeArticle
dc.typeText
tib.accessRightsopenAccess
wgl.contributorINP
wgl.subjectPhysikger
wgl.typeZeitschriftenartikelger
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