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dc.date.accessioned2024-03-02T16:50:15Z
dc.date.available2024-03-02T16:50:15Z
dc.date.created2023-07-19T11:46:11Z
dc.date.issued2023
dc.identifier.citationParaswarar Harikrishnan, Abhishek Rodal, Marie Klein, Rupert Margerit, Daniel Vercauteren, Nikki . On the motion of hairpin filaments in the atmospheric boundary layer. Physics of Fluids. 2023, 35(7)
dc.identifier.urihttp://hdl.handle.net/10852/108934
dc.description.abstractA recent work of Harikrishnan et al. [“Geometry and organization of coherent structures in stably stratified atmospheric boundary layers,” arXiv:2110.02253 (2021)] has revealed an abundance of hairpin-like vortex structures, oriented in a similar direction, in the turbulent patches of a stably stratified Ekman flow. In this study, hairpin-like structures are investigated by treating them as slender vortex filaments, i.e., a vortex filament whose diameter d is small when compared to its radius of curvature R. The corrected thin-tube model of Klein and Knio [“Asymptotic vorticity structure and numerical simulation of slender vortex filaments,” J. Fluid Mech. 284, 275 (1995)] is used to compute the motion of these filaments with the atmospheric boundary layer as a background flow. Our results suggest that the orientation of the hairpin filament in the spanwise direction is linked to its initial starting height under stable stratification, whereas no such dependency can be observed with the neutrally stratified background flow. An improved feature tracking scheme based on spatial overlap for tracking Q-criterion vortex structures on the direct numerical simulation data is also developed. It overcomes the limitation of using a constant threshold in time by dynamically adjusting the thresholds to accommodate the growth or deterioration of a feature. A comparison between the feature tracking and the filament simulation reveals qualitatively similar temporal developments. Finally, an extension of the asymptotic analysis of Callegari and Ting [“Motion of a curved vortex filament with decaying vortical core and axial velocity,” J. Appl. Math. 35, 148–175 (1978)] is carried out to include the effect of gravity. The results show that, in the regime considered here, a contribution from the gravity term occurs only when the tail of an infinitely long filament is tilted at an angle relative to the wall.
dc.languageEN
dc.publisherAmerican Institute of Physics
dc.rightsAttribution 4.0 International
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.titleOn the motion of hairpin filaments in the atmospheric boundary layer
dc.title.alternativeENEngelskEnglishOn the motion of hairpin filaments in the atmospheric boundary layer
dc.typeJournal article
dc.creator.authorParaswarar Harikrishnan, Abhishek
dc.creator.authorRodal, Marie
dc.creator.authorKlein, Rupert
dc.creator.authorMargerit, Daniel
dc.creator.authorVercauteren, Nikki
cristin.unitcode185,15,22,0
cristin.unitnameInstitutt for geofag
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode2
dc.identifier.cristin2162820
dc.identifier.bibliographiccitationinfo:ofi/fmt:kev:mtx:ctx&ctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.jtitle=Physics of Fluids&rft.volume=35&rft.spage=&rft.date=2023
dc.identifier.jtitlePhysics of Fluids
dc.identifier.volume35
dc.identifier.issue7
dc.identifier.pagecount27
dc.identifier.doihttps://doi.org/10.1063/5.0151078
dc.type.documentTidsskriftartikkel
dc.type.peerreviewedPeer reviewed
dc.source.issn1070-6631
dc.type.versionPublishedVersion
cristin.articleid076603


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