2017
DOI: 10.1063/1.5002135
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Limit cycles for the motion of finite-size particles in axisymmetric thermocapillary flows in liquid bridges

Abstract: The motion of a small spherical particle of finite size in an axisymmetric thermocapillary liquid bridge is investigated numerically and experimentally. Due to the crowding of streamlines towards the free surface and the recirculating nature of the flow, advected particles visit the free surface repeatedly. The balance between centrifugal inertia and the strong short-range repulsive forces a particle experiences near the free surface leads to an attracting limit cycle for the particle motion. The existence of … Show more

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Cited by 32 publications
(44 citation statements)
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“…We stress that such a simplified particle-boundary interaction model has been proven successful at capturing the leading-order dynamics of interaction phenomena between small particles and driving boundaries (either walls or shear surfaces). This has been confirmed by comparison with fully-resolved simulations [26,27] and experiments [28]. Moreover, recent studies show that the same non-trivial physics is predicted by employing the PSI model and more physically-sound interaction forces such as the augmented Stokes drag of [6], see [14,15,29].…”
Section: Problem Formulationsupporting
confidence: 62%
See 1 more Smart Citation
“…We stress that such a simplified particle-boundary interaction model has been proven successful at capturing the leading-order dynamics of interaction phenomena between small particles and driving boundaries (either walls or shear surfaces). This has been confirmed by comparison with fully-resolved simulations [26,27] and experiments [28]. Moreover, recent studies show that the same non-trivial physics is predicted by employing the PSI model and more physically-sound interaction forces such as the augmented Stokes drag of [6], see [14,15,29].…”
Section: Problem Formulationsupporting
confidence: 62%
“…The initial particle position is (x 0 , y 0 ) = (−0.25, 0), the Stokes number is fixed to St = 1, the particle-to-fluid density ratio is varied in the interval ∈ [0.5, 1.5] and the Strouhal number of the flow ranges in Str ∈ [0.0005, 0.1]. As shown by [26][27][28]30], ∆ is of the same order of magnitude of a, hence in the followings we set ∆ = a. All the simulations are run in dimensional form for t = 10 and Ω = 2 × 10 3 .…”
Section: Resultsmentioning
confidence: 99%
“…Due to the lack of data in the literature for Pr = 68, the basic state obtained by our code for an indeformable interface has been compared by independent calculations of F. Romanò (private communication, see also Romanò et al (2017)). All results compare very well qualitatively as well as quantitatively, even though both codes differ and different grids have been used.…”
Section: Numerical Methods and Code Verificationmentioning
confidence: 99%
“…2017; Romanò et al. 2017). In laminar micro- or millimetric three-dimensional flows, the particle–boundary interaction may lead to non-trivial accumulation phenomena such as finite-size Lagrangian coherent structures which have been observed experimentally (Schwabe, Hintz & Frank 1996; Kuhlmann et al.…”
Section: Introductionmentioning
confidence: 99%