Abstract

We present a rigorous thermodynamic treatment of irreversible binary aggregation. We construct the Smoluchowski ensemble as the set of discrete finite distributions that are reached in fixed number of merging events and define a probability measure on this ensemble, such that the mean distribution in the mean-field approximation is governed by the Smoluchowski equation. In the scaling limit this ensemble gives rise to a set of relationships identical to those of familiar statistical thermodynamics. The central element of the thermodynamic treatment is the selection functional, a functional of feasible distributions that connects the probability of distribution to the details of the aggregation model. We obtain scaling expressions for general kernels and closed-form results for the special case of the constant, sum and product kernel. We study the stability of the most probable distribution, provide criteria for the sol-gel transition and obtain the distribution in the post-gel region by simple thermodynamic arguments.

Highlights

  • Aggregation is the process of forming structures through the merging of clusters

  • Of particular interest is gelling, a condition that arises under the product kernel Ki,j = ij; it refers to the formation of a giant structure, as in polymer gels, and is manifested by the failure of the Smoluchowski equation to conserve mass

  • This process is commonly described as a phase transition, suggesting the possibility that statistical thermodynamics, a theory developed for equilibrium states of interacting particles, may perhaps be applicable in this clearly irreversible process

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Summary

Introduction

Aggregation is the process of forming structures through the merging of clusters. This generic process is encountered in a large variety of systems, from polymerization and colloidal aggregation to the clustering of social groups and the merging of galaxies. Of particular interest is gelling, a condition that arises under the product kernel Ki,j = ij; it refers to the formation of a giant structure, as in polymer gels, and is manifested by the failure of the Smoluchowski equation to conserve mass This process is commonly described as a phase transition, suggesting the possibility that statistical thermodynamics, a theory developed for equilibrium states of interacting particles, may perhaps be applicable in this clearly irreversible process. The stochastic approach views clusters as entities that merge with probabilities proportional to the aggregation kernel It was first formulated by Marcus [6] for a discrete finite population, and its formal mathematical treatment was developed by Lushnikov, who obtained solutions for certain special cases, including gelation [7,8,9,10,11].

The Smoluchowski Ensemble
Kinetics
Probabilities
Smoluchowski Equation
Partition Function and Selection Functional
Shannon Entropy
The Selection Functional
Propagation Equations
Most Probable Distribution
Thermodynamics
Gibbs Distributions
Constant Kernel
Sum Kernel
Quasi-Gibbs Kernels—The Product Kernel
Stability
Phase Splitting—The Sol-Gel Transition
Monte Carlo Simulations
Continuous Limit
Summary
Full Text
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