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dc.contributor.authorSandoval, Mario
dc.contributor.authorMarath, Navaneeth K.
dc.contributor.authorSubramanian, Ganesh
dc.contributor.authorLauga, Eric
dc.date.accessioned2017-02-21T07:02:35Z-
dc.date.available2017-02-21T07:02:35Z-
dc.date.issued2014
dc.identifier.citationSandoval, M; Marath, NK; Subramanian, G; Lauga, E, Stochastic dynamics of active swimmers in linear flows. Journal of Fluid Mechanics 2014, 742, 50-70, http://dx.doi.org/10.1017/jfm.2013.651en_US
dc.identifier.citationJournal of Fluid Mechanicsen_US
dc.identifier.citation742en_US
dc.identifier.issn0022-1120
dc.identifier.urihttps://libjncir.jncasr.ac.in/xmlui/10572/2438-
dc.descriptionRestricted Accessen_US
dc.description.abstractMost classical work on the hydrodynamics of low-Reynolds-number swimming addresses deterministic locomotion in quiescent environments. Thermal fluctuations in fluids are known to lead to a Brownian loss of the swimming direction, resulting in a transition from short-time ballistic dynamics to effective long-time diffusion. As most cells or synthetic swimmers are immersed in external flows, we consider theoretically in this paper the stochastic dynamics of a model active particle (a self-propelled sphere) in a steady general linear flow. The stochasticity arises both from translational diffusion in physical space, and from a combination of rotary diffusion and so-called run-and-tumble dynamics in orientation space. The latter process characterizes the manner in which the orientation of many bacteria decorrelates during their swimming motion. In contrast to rotary diffusion, the decorrelation occurs by means of large and impulsive jumps in orientation (tumbles) governed by a Poisson process. We begin by deriving a general formulation for all components of the long-time mean square displacement tensor for a swimmer with a time-dependent swimming velocity and whose orientation decorrelates due to rotary diffusion alone. This general framework is applied to obtain the convectively enhanced mean-squared displacements of a steadily swimming particle in three canonical linear flows (extension, simple shear and solid-body rotation). We then show how to extend our results to the case where the swimmer orientation also decorrelates on account of run-and-tumble dynamics Self-propulsion in general leads to the same long-time temporal scalings as for passive particles in linear flows but with increased coefficients. In the particular case of solid-body rotation, the effective long-time diffusion is the same as that in a quiescent fluid, and we clarify the lack of flow dependence by briefly examining the dynamics in elliptic linear flows. By comparing the new active terms with those obtained for passive particles we see that swimming can lead to an enhancement of the mean-square displacements by orders of magnitude, and could be relevant for biological organisms or synthetic swimming devices in fluctuating environmental or biological flows.en_US
dc.description.uri1469-7645en_US
dc.description.urihttp://dx.doi.org/10.1017/jfm.2013.651en_US
dc.language.isoEnglishen_US
dc.publisherCambridge Univ Pressen_US
dc.rights@Cambridge Univ Press, 2014en_US
dc.subjectMechanicsen_US
dc.subjectFluids & Plasmas Physicsen_US
dc.subjectBiological Fluid Dynamicsen_US
dc.subjectShear Flowsen_US
dc.subjectLow-Reynolds Number Locomotionen_US
dc.subjectHomogeneous Shear Flowsen_US
dc.subjectBrownian Particlesen_US
dc.subjectTumble Chemotaxisen_US
dc.subjectTaylor Dispersionen_US
dc.subjectMicroorganismsen_US
dc.subjectDiffusionen_US
dc.subjectRunen_US
dc.subjectSuspensionsen_US
dc.subjectLocomotionen_US
dc.subjectTransporten_US
dc.titleStochastic dynamics of active swimmers in linear flowsen_US
dc.typeArticleen_US
Appears in Collections:Research Articles (Ganesh Subramanian)

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