Abstract

Electrically insulating objects immersed in a weakly conducting liquid may Quincke rotate when subjected to an electric field. Experimental and theoretical investigations of this type of electrorotation typically concern rigid particles and particle-free droplets. This work provides the basic features of electric field-induced rotation of particle-covered droplets that expand the current knowledge in this area. Compared to pure droplets, we show that adding particles to the droplet interface considerably changes the parameters of electrorotation. We study in detail deformation magnitude (D), orientation (β) and rotation rate (ω) of a droplet subjected to a DC E-field. Our experimental results reveal that both the critical electric field (for electrorotation) and the rotational rate depend on droplet size, particle shell morphology (smooth vs. brush-like), and composition (loose vs. locked particles). We also demonstrate the importance of the electrical parameters of the surface particles by comparing the behavior of droplets covered by (insulating) polymeric particles and droplets covered by (non-ohmic) clay mineral particles. The knowledge acquired from the electrorotation experiments is directly translated into practical applications: (i) to form arrested droplets with shells of different permeability; (ii) to study solid-to-liquid transition of particle shells; (iii) to mix particles on shells; and (iv) to increase the formation efficiency of Pickering emulsions.

Highlights

  • Electric fields (E-fields) can rotate objects suspended in a liquid

  • Slow rotation of the particle-covered droplet was observed above 225 V mmÀ1, and from B265 V mmÀ1 the rotation rate increased nearly linearly with the increase of the E-field strength

  • We showed that the addition of particles to the droplet interface changes the parameters of electrorotation compared to those of pure droplets and solid particles

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Summary

Introduction

Electric fields (E-fields) can rotate objects suspended in a liquid. There are several different mechanisms for electro-rotation, and these may employ either static or rotating E-fields.[1,2,3,4,5,6] This work concerns rotation of particle-covered droplets that are subjected to a static and uniform E-field. The electrorotation studied here is similar to that described more than a century ago by Weiler and Quincke who observed rotation of electrically insulating particles immersed in a weakly conductive liquid.[7,8]. The theory on the rotation frequency of Quincke rotating particles was established a long time ago and has since been further developed.[9,10,11] The influence of particle shape, size and electrical properties on the rotation rate and critical E-field (at which the rotation of solid particle begins) is well described.[12,13,14]

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