Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/113320
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dc.contributorDepartment of Civil and Environmental Engineeringen_US
dc.creatorMa, Yen_US
dc.creatorMohebbi, Ren_US
dc.creatorYang, Zen_US
dc.date.accessioned2025-06-02T06:58:10Z-
dc.date.available2025-06-02T06:58:10Z-
dc.identifier.issn1070-6631en_US
dc.identifier.urihttp://hdl.handle.net/10397/113320-
dc.language.isoenen_US
dc.publisherAIP Publishing LLCen_US
dc.rights© 2025 Author(s). Published under an exclusive license by AIP Publishing.en_US
dc.rightsThis article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing. This article appeared in Yuan Ma, Rasul Mohebbi, Zhigang Yang; Blocking phenomenon induced by droplet electrocoalescence and wavy walls. Physics of Fluids 1 March 2025; 37 (3): 033629 and may be found at https://doi.org/10.1063/5.0263873.en_US
dc.titleBlocking phenomenon induced by droplet electrocoalescence and wavy wallsen_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: 马原en_US
dc.description.otherinformationAuthor name used in this publication: 杨志刚en_US
dc.identifier.spage033629-01en_US
dc.identifier.epage033629-11en_US
dc.identifier.volume37en_US
dc.identifier.issue3en_US
dc.identifier.doi10.1063/5.0263873en_US
dcterms.abstractThis study explores the impact of wavy walls and electric fields on the deformation and coalescence of droplets using a fully coupled model developed in COMSOL. The model integrates the Navier–Stokes equations, Maxwell stress tensor, and phase-field model to analyze the effects of electric field strength, wavy wall amplitude, and wavy wall wavelength. It can be found that in a cavity with flat walls and no applied electric field, droplets coalesce and descend. At low electric field strengths, droplets adhere to one sidewall, altering their descent. With an increased potential of 2000 V, droplets coalesce to form a stationary barrier layer that divides the cavity into upper and lower sections. The presence of wavy walls significantly influences droplet behavior. At A = 0.5, L = 5, and V0 = 2000 V, an inclined barrier layer form. Increasing the A enhances the influence of the wavy walls, thereby decelerating the descent of the droplets. Conversely, reduced L inhibits droplet descent. This study highlights the complex interplay between electric fields and wavy walls in controlling droplet dynamics.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationPhysics of fluids, Mar. 2025, v. 37, no. 3, 033629, p. 033629-01 - 033629-11en_US
dcterms.isPartOfPhysics of fluidsen_US
dcterms.issued2025-03-
dc.identifier.scopus2-s2.0-105001386083-
dc.identifier.eissn1089-7666en_US
dc.identifier.artn033629en_US
dc.description.validate202506 bcchen_US
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_Others-
dc.description.fundingSourceSelf-fundeden_US
dc.description.pubStatusPublisheden_US
dc.description.oaCategoryVoR alloweden_US
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