Abstract

We investigate the effect of inertial particles on the stability and decay of a prototypical vortex tube, represented by a two-dimensional Lamb–Oseen vortex. In the absence of particles, the strong stability of this flow makes it resilient to perturbations, whereby vorticity and enstrophy decay at a slow rate controlled by viscosity. Using Eulerian–Lagrangian simulations, we show that the dispersion of semidilute inertial particles accelerates the decay of the vortex tube by orders of magnitude. In this work, mass loading is unity, ensuring that the fluid and particle phases are tightly coupled. Particle inertia and vortex strength are varied to yield Stokes numbers 0.1–0.4 and circulation Reynolds numbers 800–5000. Preferential concentration causes these inertial particles to be ejected from the vortex core forming a ring-shaped cluster and a void fraction bubble that expand outwards. The outward migration of the particles causes a flattening of the vorticity distribution, which enhances the decay of the vortex. The latter is further accelerated by small-scale clustering that causes enstrophy to grow, in contrast with the monotonic decay of enstrophy in single-phase two-dimensional vortices. These dynamics unfold on a time scale that is set by preferential concentration and is two orders of magnitude lower than the viscous time scale. Increasing particle inertia causes a faster decay of the vortex. This work shows that the injection of inertial particles could provide an effective strategy for the control and suppression of resilient vortex tubes.

Highlights

  • The dispersion of heavy inertial particles in columnar vortices is a fundamental and widely occurring process

  • It is well established that particles heavier than the suspending fluid tend to be ejected out of vortical regions by a mechanism known as preferential concentration (Squires & Eaton 1990, 2014; Wang & Maxey 1993), the joint evolution of the particle phase and carrier vortical flow under two-way coupling is poorly understood

  • We investigate the effects of particle inertia on this prototypical vortex tube under strong interphase coupling due to mass loading M = 1

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Summary

Introduction

The dispersion of heavy inertial particles in columnar vortices is a fundamental and widely occurring process. Using direct numerical simulations and Lagrangian tracking, Marshall (2005) studied the one-way coupled dispersion of inertial particles in a columnar vortex enveloped by turbulence He found that inertial particles, initially dispersed within the vortex core, quickly form annular structures that swell radially outwards. To other authors, Druzhinin (1994) showed that the particles form a ring-shaped cluster that expands outwardly from the core at a rate controlled by their inertia and leaves the core depleted of particles For these weakly inertial particles, Druzhinin (1994) suggests that particle dispersion should follow a spiralling motion caused by an inward fluid momentum flux resulting from the outward particle momentum flux.

Governing equations
Fluid motion of the single-phase Lamb–Oseen vortex
Overview
Time scale of particle-laden vortex and preferential concentration
Modulation of the fluid phase
Conclusion
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