Abstract

Interaction of droplets with vortical structures is ubiquitous in nature, ranging from raindrops to a gas turbine combustor. In this work, we elucidate the mechanism of co-axial interaction of a droplet with a vortex ring of different circulation strengths ( $\varGamma = 45\text {--}161\ \textrm {cm}^2\ \textrm {s}^{-1}$ ). We focus on both the droplet and the vortex dynamics, which evolve in a spatio-temporal fashion during different stages of the interaction, as in a two-way coupled system. Vortex rings of varying circulation strengths are generated by injecting a slug of water into a quiescent water-filled chamber. Experimental techniques such as high-speed particle image velocimetry, planner laser-induced fluorescence imaging and high-speed shadowgraphy are used in this work. In the droplet dynamics, different regimes of interaction are identified, including deformation (regime-I), stretching and engulfment (regime-II) and breakup of the droplet (regime-III). Each interaction regime is explained using existing theoretical models that closely match the experimental data. In the vortex dynamics, we compare the interaction's effect on different characteristics of the vortex rings, such as pressure and the vorticity distribution, circulation strength, total energy and enstrophy variation with time. It is found that the interaction leads to a reduction in these parameters.

Highlights

  • A vortex ring, known as a toroidal ring, is a torus-shaped confined region of vorticity embedded in a fluid medium

  • The effect of interaction on the vortex dynamics will be presented, where we will discuss the variation of vorticity distribution, circulation strength, total energy and enstrophy and translation speed of the vortex ring, and the results are compared with the reference case of no interaction

  • If the pressure force is greater than the surface tension force, droplet deformation occurs

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Summary

Introduction

A vortex ring, known as a toroidal ring (three-dimensional case), is a torus-shaped confined region of vorticity embedded in a fluid medium. Kolmogorov (1949) and Hinze (1955) initially investigated the droplet break up in a turbulent flow Later, it was further studied by various researchers using theoretical (Luo & Svendsen 1996; Wang, Wang & Jin 2003; Solsvik & Jakobsen 2016) and experimental techniques (Konno et al 1980; Eastwood et al 2004; Andersson & Andersson 2006). Interaction studies with deformable dispersed phases of larger diameter (bubble and droplet) are less frequent in the existing literature (Higuera 2004; Revuelta 2010; Jha & Govardhan 2015; Zednikova et al 2019).

Flow set-up
Backlight imaging set-up
PIV and LIF imaging
Experimental conditions
Theoretical model
90 Case V 60
Regime-III: droplet breakup
Results and discussion
Droplet dynamics regime-I: droplet deformation
Droplet dynamics regime-II: droplet stretching and engulfment
Case V
Droplet dynamics regime-III: droplet breakup
Vortex dynamics: effect on vorticity distribution and circulation strength
12 Case V 10 8 6 4 2 0
Summary and conclusions
Full Text
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