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Order-disorder transitions in a sheared many body system (1507.04926v2)

Published 17 Jul 2015 in cond-mat.soft, nlin.CD, and physics.flu-dyn

Abstract: Motivated by experiments on sheared suspensions that show a transition between ordered and disordered phases, we here study the long-time behavior of a sheared and overdamped 2-d system of particles interacting by repulsive forces. As a function of interaction strength and shear rate we find transitions between phases with vanishing and large single-particle diffusion. In the phases with vanishing single-particle diffusion, the system evolves towards regular lattices, usually on very slow time scales. Different lattices can be approached, depending on interaction strength and forcing amplitude. The disordered state appears in parameter regions where the regular lattices are unstable. Correlation functions between the particles reveal the formation of shear bands. In contrast to single particle densities, the spatially resolved two-particle correlation functions vary with time and allow to determine the phase within a period. As in the case of the suspensions, motion in the state with low diffusivity is essentially reversible, whereas in the state with strong diffusion it is not.

Summary

  • The paper investigates order-disorder transitions in a 2D sheared many-body system, linking transitions to single-particle diffusion changes based on varying shear rates and interaction strengths.
  • Numerical simulations reveal that the system transitions from ordered lattice structures to a disordered state with heightened diffusion as the shear rate increases past a critical value.
  • Floquet stability analysis confirms that ordered states lose stability with increasing shear rate, providing a theoretical basis for the observed macroscopic transition behavior.

Order-Disorder Transitions in a Sheared Many-Body System

The paper presents a detailed investigation into the behaviors observed in a two-dimensional overdamped many-body system subjected to shear forces. The system uses particles interacting via repulsive forces and demonstrates transitions between ordered and disordered states based on varying shear rates and interaction strengths. This paper is motivated by experiments on sheared suspensions that reveal similar transitions in real-world systems.

Key Research Components and Findings

This research utilizes a simplified model to analyze the long-term dynamics of the system, focusing on single-particle diffusion as a key indicator of the phase transition. The authors observe that at certain thresholds of shear rate and interaction strength, the system exhibits significant differences in diffusivity, marking transitions between ordered (reversible) and disordered (irreversible) states. In the reversible states, particles tend towards regular lattice formations, while in the irreversible state, particles diffuse chaotically.

Numerical Results

The authors' simulations show critical regions where stable ordered states become unstable and correlate these results with observations from stroboscopic maps and correlation functions. Numerical experiments reveal:

  • Ordered States: At low shear rates and interaction strengths, particles arrange into crystalline structures, either hexagonal or rectangular, depending on the parameters.
  • Disordered States: As shear rate increases beyond a critical value, the system transitions to a disordered state characterized by heightened diffusion.
  • Diffusion Characteristics: Diffusivity along the shear direction substantially exceeds that in the perpendicular direction, a phenomenon attributable to advection-diffusion coupling, with implications on the understanding of shear flow interactions in particle systems.
  • Correlation Functions: Spatial correlation analyses highlight anisotropic particle arrangements in ordered states and a dilution in correlations for disordered states.

Stability Analysis

Through Floquet analysis, the stability of various particle lattice configurations is assessed. The stability analysis aligns well with numerical observations, indicating that ordered states lose stability as the shear rate increases past a certain threshold. This approach ties the macroscopic transition behavior to underlying microscopic stability changes.

Implications and Future Directions

The paper's findings broaden the understanding of phase transitions in non-equilibrium many-body systems under shear. The methodologies and insights gained could inform future research in complex fluid dynamics, materials science, and related fields where similar transition phenomena are observed. Future research might explore broader interaction models or additional external forces, allowing for the paper of more complex or realistic physical systems. Further investigation into the role of long-range interactions and modifications in system boundary conditions might yield additional insights into the intricate balance between order and chaos in physical systems under shear.

By marrying simulations with theoretical stability analyses, this paper provides a comprehensive look into the complex behaviors of sheared many-body systems, paving the way for deeper insights into the dynamics of materials subjected to external stresses.

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