2015
DOI: 10.1063/1.4916583
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Caustics and clustering in the vicinity of a vortex

Abstract: We study the formation of caustics in vortex-dominated flows. We find that only particles starting within a critical distance of a vortex which scales as the square roots of the particle inertia and the circulation can form sling caustics. We show that particles starting in an annular region around this critical radius contribute the densest clusters in the flow. The large density spikes occurring for such particles, even at small inertia, are indicative that these particles will experience large collision rat… Show more

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Cited by 39 publications
(42 citation statements)
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“…Close to a point vortex, upon neglecting the Basset history, the dynamics of particles has been shown to obey a boundary-layer structure (Ravichandran & Govindarajan 2015;Deepu et al 2017), where particles initially located within a critical radius r c are able to form caustics and evacuate the vicinity of the vortex rapidly, whereas particles initially outside this radius do not form caustics, and so their dynamics may be represented by a velocity field. We define caustics as space-time points where two particles can exist simultaneously with different velocities.…”
mentioning
confidence: 99%
“…Close to a point vortex, upon neglecting the Basset history, the dynamics of particles has been shown to obey a boundary-layer structure (Ravichandran & Govindarajan 2015;Deepu et al 2017), where particles initially located within a critical radius r c are able to form caustics and evacuate the vicinity of the vortex rapidly, whereas particles initially outside this radius do not form caustics, and so their dynamics may be represented by a velocity field. We define caustics as space-time points where two particles can exist simultaneously with different velocities.…”
mentioning
confidence: 99%
“…) We see clearly that starting from an initial profile in which particles are uniformly distributed in space, the particles evacuate rapidly from regions close to the core of the vortex. (The case of σ = 0 is validated against Ravichandran and Govindarajan [25].) Therefore, at some later time (t = 0.6τ η ), Φ is essentially 0 at small values of r before sharply peaking at r .…”
Section: Resultsmentioning
confidence: 87%
“…A scale-free version (again following the scaling used in Ref. [25]) where the dependence on the Taylor Reynolds number is apparent is shown in the Appendix. The decrease in the critical Stokes number with increasing stretch- FIG.…”
Section: Resultsmentioning
confidence: 99%
“…They can also attain relative velocities much larger than that of the underlying flow. Dubbed the sling effect [41], these events correspond to the formation of singularities or caustics in the particle velocity field [42,43]. Although clustering and caustics have been tied to the centrifugal ejection of heavy particles out of vortices, they also occur in smooth random flows that are devoid of structure [44][45][46][47][48].…”
mentioning
confidence: 99%
“…One possible explanation is provided by preferential concentration: Heavy particles are centrifuged out of rotational regions, and thus tend to accumulate in straining zones just outside vortices [43]. This causes the number density to increase in straining regions, at the expense of vortical zones, as shown in Fig.…”
mentioning
confidence: 99%