Physical interpretation of the partition function for colloidal clusters
arXiv:1806.00155 · doi:10.1103/PhysRevE.98.032608
Abstract
Colloidal clusters consist of small numbers of colloidal particles bound by weak, short-range attractions. The equilibrium probability of observing a cluster in a particular geometry is well-described by a statistical mechanical model originally developed for molecules. To explain why this model fits experimental data so well, we derive the partition function classically, with no quantum mechanical considerations. Then, by comparing and contrasting the derivation in particle coordinates with that in center-of-mass coordinates, we physically interpret the terms in the center-of-mass formulation, which is equivalent to the high-temperature partition function for molecules. We discuss, from a purely classical perspective, how and why cluster characteristics such as the symmetry number, moments of inertia, and vibrational frequencies affect the equilibrium probabilities.
References in corpus (10)
- Two-Dimensional Clusters of Colloidal Spheres: Ground States, Excited States, and Structural Rearrangements
- Deriving Finite Sphere Packings
- Enumerating rigid sphere packings
- Structure of finite sphere packings via exact enumeration: Implications for colloidal crystal nucleation
- Geometric frustration in small colloidal clusters
- Testing the Foundations of Classical Entropy: Colloid Experiments
- Minimal energy packings and collapse of sticky tangent hard-sphere polymers
- Sticky-sphere clusters
- Structure and dynamics of model colloidal clusters with short-range attractions
- Free energy of singular sticky-sphere clusters