Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/95592
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dc.contributorDepartment of Mechanical Engineeringen_US
dc.creatorQin, Men_US
dc.creatorTang, Cen_US
dc.creatorTong, Sen_US
dc.creatorZhang, Pen_US
dc.creatorHuang, Zen_US
dc.date.accessioned2022-09-22T06:14:01Z-
dc.date.available2022-09-22T06:14:01Z-
dc.identifier.issn0301-9322en_US
dc.identifier.urihttp://hdl.handle.net/10397/95592-
dc.language.isoenen_US
dc.publisherPergamon Pressen_US
dc.rights© 2019 Elsevier Ltd. All rights reserved.en_US
dc.rights© 2019. This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/.en_US
dc.rightsThe following publication Qin, M., Tang, C., Tong, S., Zhang, P., & Huang, Z. (2019). On the role of liquid viscosity in affecting droplet spreading on a smooth solid surface. International Journal of Multiphase Flow, 117, 53-63 is available at https://doi.org/10.1016/j.ijmultiphaseflow.2019.05.002en_US
dc.subjectDroplet impacten_US
dc.subjectMaximum spreading diameteren_US
dc.subjectNon-monotonic dependenceen_US
dc.subjectViscosity effecten_US
dc.titleOn the role of liquid viscosity in affecting droplet spreading on a smooth solid surfaceen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage53en_US
dc.identifier.epage63en_US
dc.identifier.volume117en_US
dc.identifier.doi10.1016/j.ijmultiphaseflow.2019.05.002en_US
dcterms.abstractThe role of liquid viscosity on droplet spreading behavior upon impacting on a smooth stainless steel surface has been experimentally investigated. Results show the droplet spreading dynamics with increasing viscosity (characterized by the Ohnesorge number, Oh)exhibits complex dependence on the impact inertia (characterized by Weber number, We). Specifically, for a small impact inertia (We<30), the droplet oscillates in the vertical direction around the maximum height Ha. The non-dimensional maximum diameter βmax first increases and then decreases with increasing Oh, and this non-monotonic phenomenon has not been reported previously. For an intermediate impact inertia (60<We<240), the droplet has no oscillation after it spreads to βmax, and it has the form of a rim-bounded lamella. Although βmax shows a monotonic decrease with increasing Oh, some unsmooth disturbance around the rim occurs only at intermediate Oh. For a higher impact inertia (We>240), droplet splashing emerges and then vanishes with increasing Oh, although βmax still decreases monotonically. All the observed phenomena imply that liquid viscosity may have a dual role in affecting the droplet spreading, which previous models of βmax do not take into account.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationInternational journal of multiphase flow, Aug. 2019, v. 117, p. 53-63en_US
dcterms.isPartOfInternational journal of multiphase flowen_US
dcterms.issued2019-08-
dc.identifier.scopus2-s2.0-85065546938-
dc.identifier.eissn1879-3533en_US
dc.description.validate202209_bcwwen_US
dc.description.oaAccepted Manuscripten_US
dc.identifier.FolderNumberME-0424-
dc.description.fundingSourceRGCen_US
dc.description.fundingSourceOthersen_US
dc.description.fundingTextThe Hong Kong Polytechnic Universityen_US
dc.description.pubStatusPublisheden_US
dc.identifier.OPUS14479277-
dc.description.oaCategoryGreen (AAM)en_US
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