Please use this identifier to cite or link to this item: https://doi.org/10.1002/nme.3182
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dc.titleA three-dimensional hybrid meshfree-Cartesian scheme for fluid-body interaction
dc.contributor.authorYu, P.
dc.contributor.authorYeo, K.S.
dc.contributor.authorShyam Sundar, D.
dc.contributor.authorAng, S.J.
dc.date.accessioned2014-06-17T06:10:03Z
dc.date.available2014-06-17T06:10:03Z
dc.date.issued2011-10-28
dc.identifier.citationYu, P., Yeo, K.S., Shyam Sundar, D., Ang, S.J. (2011-10-28). A three-dimensional hybrid meshfree-Cartesian scheme for fluid-body interaction. International Journal for Numerical Methods in Engineering 88 (4) : 385-408. ScholarBank@NUS Repository. https://doi.org/10.1002/nme.3182
dc.identifier.issn00295981
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/59318
dc.description.abstractA numerical method based on a hybrid meshfree-Cartesian grid is developed for solving three-dimensional fluid-solid interaction (FSI) problems involving solid bodies undergoing large motion. The body is discretized and enveloped by a cloud of meshfree nodes. The motion of the body is tracked by convecting the meshfree nodes against a background of Cartesian grid points. Spatial discretization of second-order accuracy is accomplished by the combination of a generalized finite difference (GFD) method and conventional finite difference (FD) method, which are applied to the meshfree and Cartesian nodes, respectively. Error minimization in GFD is carried out by singular value decomposition. The discretized equations are integrated in time via a second-order fractional step projection method. A time-implicit iterative procedure is employed to compute the new/evolving position of the immersed bodies together with the dynamically coupled solution of the flow field. The present method is applied on problems of free falling spheres and tori in quiescent flow and freely rotating spheres in simple shear flow. Good agreement with published results shows the ability of the present hybrid meshfree-Cartesian grid scheme to achieve good accuracy. An application of the method to the self-induced propulsion of a deforming fish-like swimmer further demonstrates the capability and potential of the present approach for solving complex FSI problems in 3D. © 2011 John Wiley & Sons, Ltd.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1002/nme.3182
dc.sourceScopus
dc.subjectArbitrary Lagrangian-Eulerian formulation
dc.subjectFluid-structure interaction
dc.subjectGeneralized finite difference method
dc.subjectMeshfree method
dc.subjectSelf-propulsion
dc.subjectSwimming
dc.typeArticle
dc.contributor.departmentMECHANICAL ENGINEERING
dc.description.doi10.1002/nme.3182
dc.description.sourcetitleInternational Journal for Numerical Methods in Engineering
dc.description.volume88
dc.description.issue4
dc.description.page385-408
dc.description.codenIJNMB
dc.identifier.isiut000295226600005
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