Kinetics of isotropic to string-like phase switching in electrorheological fluids of nanocubes

TL;DR

This study uses simulations and microrheology to explore how dielectric nanocubes in electrorheological fluids form string-like clusters under electric fields, revealing two distinct switching mechanisms and anisotropic viscoelastic behavior.

Contribution

It introduces a detailed kinetic analysis of the isotropic to string-like phase transition in nanocube-based electrorheological fluids, highlighting two mechanisms and anisotropic viscoelasticity.

Findings

String-like clusters form at high field intensities.

Two mechanisms govern the phase switching: nucleation and merging/separation.

Electric field induces anisotropic viscoelastic properties.

Abstract

Applying an electric field to polarisable colloidal particles, whose permittivity differs from that of the dispersing medium, generates induced dipoles that promote the formation of string-like clusters and ultimately alter the fluid mechanical and rheological properties. Complex systems of this kind, whose electric-field-induced rheology can be manipulated between that of viscous and elastic materials, are referred to as electrorheological fluids. By dynamic Monte Carlo simulations, we investigate the dynamics of self-assembly of dielectric nanocubes upon application of an electric field. Switching the field on induces in-particle dipoles and, at sufficiently large field intensity, leads to stringlike clusters of variable length across a spectrum of volume fractions. The kinetics of switching from the isotropic to the string-like state suggests the existence of two mechanisms, the first related to the nucleation of chains and the second to the competition between further merging and separation. We characterise the transient unsteady state by following the chain length distribution and analysing the probability of transition of nanocubes from one chain to another over time. Additionally, we employ passive microrheology to gain an insight into the effect of the electric field on the viscoelastic response of our model fluid. Not only do we observe that it becomes more viscoelastic in the presence of the field, but also that its viscoelasticity assumes an anisotropic signature, with both viscous and elastic moduli in planes perpendicular to the external field being larger than those along it.