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Updated: Aug 11, 2026

Spatial Separation of Molecular Conformers and Clusters
Published on: January 9, 2014
Flocculation and percolation in reversible cluster-cluster aggregation
S Babu1, M Rottereau, T Nicolai
1Polymères Colloïdes Interfaces, UMR 6120 CNRS - Université du Maine, 72085, Le Mans Cedex 9, France.
Abstract:
Off-lattice dynamic Monte-Carlo simulations were done of reversible cluster-cluster aggregation for spheres that form rigid bonds at contact. The equilibrium properties were found to be determined by the life time of encounters between two particles (te). te is a function not only of the probability to form or break a bond, but also of the elementary step size of the Brownian motion of the particles. In the flocculation regime the fractal dimension of the clusters is df=2.0 and the size distribution has a power law decay with exponent tau=1.5. At larger values of te transient gels are formed. Close to the percolation threshold the clusters have a fractal dimension df=2.7 and the power law exponent of the size distribution is tau=2.1. The transition between flocculation and percolation occurs at a characteristic weight average aggregation number that decreases with increasing volume fraction.
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