Abstract

In colloidal systems, Brownian motion emerges from the massive separation of time and length scales associated to characteristic dynamics of the solute and solvent constituents. This separation of scales produces several temporal regimes in the colloidal dynamics when combined with the effects of the interaction between the particles, confinement conditions, and state variables, such as density and temperature. Some examples are the short- and long-time regimes in two- and three-dimensional open systems and the diffusive and sub-diffusive regimes observed in the single-file dynamics along a straight line. This work studies the way in which a confining geometry induces new time scales. We report on the dynamics of interacting colloidal particles moving along a circle by combining a heuristic theoretical analysis of the involved scales, Brownian Dynamics computer simulations, and video-microscopy experiments with paramagnetic colloids confined to lithographic circular channels subjected to an external magnetic field. The systems display four temporal regimes in this order: one-dimensional free diffusion, single-file sub-diffusion, free-cluster rotational diffusion, and the expected saturation due to the confinement. We also report analytical expressions for the mean-square angular displacement and crossover times obtained from scaling arguments, which accurately reproduce both experiments and simulations. Our generic approach can be used to predict the long-time dynamics of many other confined physical systems.

Highlights

  • Diffusion is one of the most common mechanisms used by nature to dissipate equilibrium density fluctuations, where the Brownian motion of colloidal particles represents a fascinating case [1]

  • We report on the dynamics of interacting colloidal particles moving along a circle by combining a heuristic theoretical analysis of the involved scales, Brownian dynamics computer simulations, and video-microscopy experiments with paramagnetic colloids confined to lithographic circular channels subjected to an external magnetic field

  • By combining video-microscopy experiments performed with paramagnetic colloidal particles confined to lithographic circular microchannels subjected to an external magnetic field with the EM algorithm for curved manifolds implemented for the paramagnetic colloids confined to a circle, we unravel the rich dynamical behavior of interacting colloidal systems that emerges due to the geometric confinement

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Summary

INTRODUCTION

Diffusion is one of the most common mechanisms used by nature to dissipate equilibrium density fluctuations, where the Brownian motion of colloidal particles represents a fascinating case [1] It exhibits a rich dynamical scenario in an extended time window due to the enormous separation of the characteristic time and length scales of solute and solvent constituents, combined with the effects of the interaction between the particles, the confinement conditions, and the state variables such as density and temperature [2,3]. By combining video-microscopy experiments performed with paramagnetic colloidal particles confined to lithographic circular microchannels subjected to an external magnetic field with the EM algorithm for curved manifolds implemented for the paramagnetic colloids confined to a circle, we unravel the rich dynamical behavior of interacting colloidal systems that emerges due to the geometric confinement.

EXPERIMENTAL SETUP
BROWNIAN DYNAMICS SIMULATIONS ON THE CIRCLE AND SUPERPARAMAGNETIC POTENTIAL
EXPERIMENTS VS
TIME SCALES FROM THE MSAD
CROSSOVER TIMES
ASYMPTOTIC BEHAVIOR
VIII. CONCLUDING REMARKS
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