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dc.contributor.authorWang, G
dc.contributor.authorLiu, Y
dc.contributor.authorLiu, C
dc.date.accessioned2023-12-04T08:38:09Z
dc.date.issued2023-11-30
dc.date.updated2023-12-01T19:35:29Z
dc.description.abstractImpact behavior in a fluidic environment is an inevitable phenomenon in multibody systems. This investigation studies the motion of a contact body in an unbounded and incompressible Newtonian viscous fluid. In allusion to the physical impact in immersed fluid, a dissipated coefficient is introduced to describe the dissipated energy caused by the hydrodynamic forces, including the drag force, added mass force, and history force. To attain the fluid damping factor during impact, the kinetic energy corresponding to the physical impact has four discrepant destinations at the end of the compression phase. According to this principle, a new fluid damping factor is derived based on the energy conservation during impact for simultaneously depicting the coupling between liquid and solid and the coupling between solid and solid. More importantly, to determine the coefficient of restitution (CoR) corresponding to the actual physical impact, a new CoR is proposed according to the definitions of dry and wet CoRs. Subsequently, since both compression and recovery phases happen in the presence of hydrodynamic forces, fluid damping force should be imposed on the Hertz contact model. Consequently, a new contact force model with a fluid damping factor tailored for immersed collision events is proposed. Although the viscosity of the fluid is not explicitly exhibited in the hysteresis damping loop from the new contact force model, the effect of fluid on the immersed collision cannot be neglected, especially for the initial distance of contact bodies. Finally, the rationality and correctness of the proposed model are validated by the reference solution obtained from the solitary wave propagation of a horizontal one-dimension granular chain.en_GB
dc.format.extent114292-114292
dc.identifier.citationVol. 178, article 114292en_GB
dc.identifier.doihttps://doi.org/10.1016/j.chaos.2023.114292
dc.identifier.urihttp://hdl.handle.net/10871/134714
dc.identifierORCID: 0000-0003-3867-5137 (Liu, Yang)
dc.identifierScopusID: 55199382800 (Liu, Yang)
dc.identifierResearcherID: ABD-4124-2021 | K-1976-2015 (Liu, Yang)
dc.language.isoenen_GB
dc.publisherElsevieren_GB
dc.rights.embargoreasonUnder embargo until 30 November 2024 in compliance with publisher policyen_GB
dc.rights © 2023 Elsevier Ltd. This version is made available under the CC-BY-NC-ND 4.0 license: https://creativecommons.org/licenses/by-nc-nd/4.0/  en_GB
dc.subjectFluid damping factoren_GB
dc.subjectHydrodynamic forceen_GB
dc.subjectCoefficient of restitutionen_GB
dc.subjectImmersed collisionen_GB
dc.titleDevelopment of a contact force model with a fluid damping factor for immersed collision eventsen_GB
dc.typeArticleen_GB
dc.date.available2023-12-04T08:38:09Z
dc.identifier.issn0960-0779
exeter.article-number114292
dc.descriptionThis is the author accepted manuscript. the final version is available from Elsevier via the DOI in this recorden_GB
dc.descriptionData availability: Data will be made available on request.en_GB
dc.identifier.journalChaos, Solitons and Fractalsen_GB
dc.rights.urihttps://creativecommons.org/licenses/by-nc-nd/4.0/en_GB
dcterms.dateAccepted2023-11-16
rioxxterms.versionAMen_GB
rioxxterms.licenseref.startdate2023-11-30
rioxxterms.typeJournal Article/Reviewen_GB
refterms.dateFCD2023-12-04T08:33:16Z
refterms.versionFCDAM
refterms.dateFOA2024-11-30T00:00:00Z
refterms.panelBen_GB


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 © 2023 Elsevier Ltd. This version is made available under the CC-BY-NC-ND 4.0 license: https://creativecommons.org/licenses/by-nc-nd/4.0/  
Except where otherwise noted, this item's licence is described as  © 2023 Elsevier Ltd. This version is made available under the CC-BY-NC-ND 4.0 license: https://creativecommons.org/licenses/by-nc-nd/4.0/