Abstract

Reversible aggregation of purely short-ranged attractive colloidal particles leads to the formation of clusters with a fractal dimension that only depends on the second virial coefficient. The addition of a long-ranged repulsion to the potential modifies the way in which the particles aggregate into clusters and form intermediate range order structures, and have a strong influence on the dynamical and rheological properties of colloidal dispersions. The understanding of the effect of a long-ranged repulsive potential on the aggregation mechanisms is scientifically and technologically important for a large variety of physical, chemical and biological systems, including concentrated protein solutions. In this work, the equilibrium cluster morphology of particles interacting through a short-ranged attraction plus a long-ranged repulsion is extensively studied by means of Monte Carlo computer simulations. Our findings point out that the addition of the repulsion affects the resulting cluster morphology and allows one to have a full control on the compactness or fractal dimension of the aggregates at a given thermodynamic condition. This allows us to manipulate the reversible aggregation process and, therefore, to finely tune the resulting building blocks of materials at large length scales.

Highlights

  • Many body systems composed of particles interacting via a short-range attraction and a long-range repulsion (SALR) have attracted attention in the past decade due to their rich phase behavior not observed for systems interacting with purely attractive potentials

  • The competition between attraction and repulsion over different length scales makes possible to have different phase diagrams depending on the parameters that control both the range and strength of each potential feature. [17] presented an empirical classification for systems with competing interactions based on the range of the repulsion and attraction

  • We focus on the cluster morphology of type I systems, since the features of the interaction are more similar to the estimated potential for colloidal systems and protein solutions, see for example references [2, 4, 5, 20,21,22,23]

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Summary

INTRODUCTION

Many body systems composed of particles interacting via a short-range attraction and a long-range repulsion (SALR) have attracted attention in the past decade due to their rich phase behavior not observed for systems interacting with purely attractive potentials One of these is the clustered fluid phase resulting from the frustration of the gas-liquid separation. Cluster Morphology of Colloidal Systems dispersed fluid, clustered fluid, and percolated states One difference of these two types of systems is that type I is believed to present a gas-liquid separation below the cluster temperature if the repulsion range is short enough, as is speculated by [17]. In a similar spirit [10], proposed a generalized phase diagram for particles with competing interactions after studying type I and II systems through Monte Carlo computer simulations.

COMPETING INTERACTION POTENTIAL AND MONTE CARLO COMPUTER SIMULATIONS
PHASE DIAGRAM
CLUSTER MORPHOLOGY
CONCLUSION
Findings
DATA AVAILABILITY STATEMENT
Full Text
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