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dc.contributor.authorMoebius, Matthiasen
dc.contributor.authorStamenov, Plamenen
dc.contributor.authorVenkatesan, Munuswamyen
dc.contributor.authorCoey, Johnen
dc.date.accessioned2023-01-16T16:52:22Z
dc.date.available2023-01-16T16:52:22Z
dc.date.issued2022en
dc.date.submitted2022en
dc.identifier.citationSruthy Poulose, Jennifer A Quirke, Plamen Stamenov, Matthias E. M�bius, J. M. D. Coey, Deformation and necking of liquid droplets in a magnetic field., Physics of Fluids, 2022en
dc.identifier.otherYen
dc.descriptionPUBLISHEDen
dc.description.abstractPendant droplets of water and paramagnetic solutions are studied in the presence of uniform and nonuniform magnetic fields produced by small permanent magnet arrays, both in static conditions and during dynamic pinch-off. Static measurements of the droplet shape are analyzed in terms of an apparent surface tension γapp or an effective density ρeff. The change of surface tension of deionized water in a uniform field of 450 mT is insignificant, 0.19 ± 0.21 mNm−1. Measurements on droplets of compensated zero-susceptibility solutions of Cu2+, Mn2+, and Dy3+, where the shape is unaffected by any magnetic body force, show changes of surface tension of about −1% in 500 mT. Magnetic field gradients of up to 100 T2 m−1 deform the droplets and lead to changes of ρeff that are negative for diamagnetic solutions (buoyancy effect) and positive for paramagnetic solutions. The droplet profile of strongly paramagnetic 0.1 molar DyCl3 solution is analyzed, treating the nonuniform vertical field gradient as a spatial variation of gravity. The influence of Maxwell stress on the droplet shape is discussed. In dynamic measurements, the droplet shape at pinch-off is recorded by high-speed photography and analyzed in terms of a relative change of dynamic surface tension in the presence of a magnetic field. The surface-tension-dependent prefactor of the scaling law that governs the pinch-off dynamics shows no difference for pure water or 0.11 M DyCl3 solutions in the field. The nonuniform field has no influence in the pinch-off region because the filament diameter is much less than the capillary length.en
dc.language.isoenen
dc.relation.ispartofseriesPhysics of Fluidsen
dc.relation.urihttps://doi.org/10.1063/5.0119614en
dc.rightsYen
dc.subjectMicrogravityen
dc.subjectg-factoren
dc.subjectOptical imagingen
dc.subjectMagnetic susceptibilityen
dc.subjectMagnetic fieldsen
dc.subjectGravitational forceen
dc.subjectMaxwell equationsen
dc.subjectSurface wavesen
dc.subjectCapillary flowsen
dc.titleDeformation and necking of liquid droplets in a magnetic field.en
dc.typeJournal Articleen
dc.type.supercollectionscholarly_publicationsen
dc.type.supercollectionrefereed_publicationsen
dc.identifier.peoplefinderurlhttp://people.tcd.ie/mobiusmen
dc.identifier.peoplefinderurlhttp://people.tcd.ie/venkatemen
dc.identifier.peoplefinderurlhttp://people.tcd.ie/stamenpen
dc.identifier.peoplefinderurlhttp://people.tcd.ie/jcoeyen
dc.identifier.rssinternalid247651en
dc.identifier.doihttp://dx.doi.org/10.1063/5.0119614en
dc.rights.ecaccessrightsopenAccess
dc.relation.sourceAmerican Institute of Physicsen
dc.relation.citesCitesen
dc.subject.TCDTagApplied physicsen
dc.subject.TCDTagCondensed matter, electronic, magnetic and superconductive propertiesen
dc.subject.TCDTagMagnetism and spin electronicsen
dc.subject.TCDTagNanotechnologyen
dc.relation.sourceurihttps://aip.scitation.org/doi/10.1063/5.0119614en
dc.identifier.orcid_id0000-0002-5509-8725en
dc.status.accessibleNen
dc.contributor.sponsorMarie Curieen
dc.contributor.sponsorGrantNumberContract No. 766007en
dc.contributor.sponsorScience Foundation Ireland (SFI)en
dc.contributor.sponsorGrantNumber17/CDA/4704en
dc.contributor.sponsorScience Foundation Ireland (SFI)en
dc.contributor.sponsorGrantNumber16/IA/4534 ZEMSen
dc.contributor.sponsorScience Foundation Ireland (SFI)en
dc.contributor.sponsorGrantNumber12/RC/2278 AMBERen
dc.identifier.urihttp://hdl.handle.net/2262/101985


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