Nonheating ozone suppression in pulsed air discharges: role of pulse duration and repetition rate

dc.bibliographicCitation.articleNumber394003
dc.bibliographicCitation.firstPage394003
dc.bibliographicCitation.issue39
dc.bibliographicCitation.journalTitleJournal of Physics D: Applied Physics
dc.bibliographicCitation.volume54
dc.contributor.authorPark, Sanghoo
dc.contributor.authorKim, Jinwoo
dc.contributor.authorLee, Hyungyu
dc.contributor.authorHan, Duksun
dc.contributor.authorPark, Seungil
dc.contributor.authorKim, Seong Bong
dc.contributor.authorChoe, Wonho
dc.date.accessioned2025-01-28T08:47:37Z
dc.date.available2025-01-28T08:47:37Z
dc.date.issued2021
dc.description.abstractFacilitating the separate production of ozone (O3) and nitrogen oxides (NO x ) in air discharges without a thermal process is of most merit in diversifying plasma technology; in particular, it is a primary requirement in certain cold, heat-sensitive plasma applications. Here, we propose a new method of nonheating ozone suppression in air discharges. The present work demonstrates that controlling the plasma chemical kinetics by adjusting the duration (width) and/or repetition frequency of the high-voltage DC pulse is effective in suppressing ozone formation in a surface dielectric barrier discharge in static ambient air. The temporal development of each oxygen- and nitrogen-related species in air discharge is complicated and shows different trends in the time range <10 µs; relatively long-lived O3 and NO x are strongly governed by the temporal behavior of short-lived reactive species, such as excited N2(A) and N2(v). To quantify time-varying O3 and NO x, an in situ UV absorption spectroscopy is applied to our gas-tight plasma reactor, which is operated in air at 21 C. With a fixed frequency at 10 kHz and decreasing pulse duration from 10 μs to 0.18 μs, ozone is quenched faster in the plasma reactor, resulting in an irreversible chemical mode transition from an O3- to NO-rich environment. From a different set of experiment (with a 200 ns pulse duration and a frequency range of 1-10 kHz), we can conclude that the off-pulse period also plays a crucial role in the temporal evolution of O3 and NO x ; the larger the applied driving frequency is, the earlier the ozone-free phenomenon appears over the discharge time. Our findings represent a breakthrough in expanding the usage of air discharges and their application in various fields of interest.eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/18543
dc.identifier.urihttps://doi.org/10.34657/17563
dc.language.isoeng
dc.publisherBristol : IOP Publ.
dc.relation.doihttps://doi.org/10.1088/1361-6463/ac113b
dc.relation.essn1361-6463
dc.relation.issn0022-3727
dc.rights.licenseCC BY 4.0 Unported
dc.rights.urihttps://creativecommons.org/licenses/by/4.0
dc.subject.ddc530
dc.subject.otherair dischargeeng
dc.subject.otherdielectric barrier dischargeeng
dc.subject.othernanosecond pulseeng
dc.subject.othernitrogen oxideseng
dc.subject.otherozoneeng
dc.subject.otherozone-free phenomenoneng
dc.subject.otherplasma chemistryeng
dc.titleNonheating ozone suppression in pulsed air discharges: role of pulse duration and repetition rateeng
dc.typeArticle
dc.typeText
tib.accessRightsopenAccess
wgl.contributorINP
wgl.subjectPhysikger
wgl.typeZeitschriftenartikelger
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