Abstract

Applying an unsteady magnetic field to a 2D nonvibrating magnetic granular system induces a random motion in the steel beads with characteristics analogous to that of molecules in a fluid. We investigate the structural characteristics of the solid-like structures generated by different quenching conditions. The applied field is generated by the superposition of a constant field and a collinear sinusoidal field. The system reaches a quasi steady state in which the effective temperature is proportional to the amplitude of the applied field. By reducing the effective temperature at different rates, different cooling rates are produced. A slight inclination of the surface allows us to investigate the effects of small particle concentration gradients. The formation of a wide and rich variety of condensed solid structures, from gel-like and glass-like structures up to crystalline structures, is observed and depends on the cooling rate. We focus our attention on the crystallization process and found this process to be a collective phenomenon. We discuss our results in terms of the measured time evolution of the mean squared displacement, the effective diffusion coefficient, and the radial distribution function.

Highlights

  • When a liquid is cooled beyond a certain temperature, it transforms into a solid body

  • We have previously studied the conditions in which a nonvibrating granular magnetic system can be fluidized by magnetic interactions induced by the application of an unsteady magnetic field[15,16,17,18]

  • We demonstrated that one can control the effective temperature of the system by varying the intensity of the applied magnetic field

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Summary

Introduction

When a liquid is cooled beyond a certain temperature, it transforms into a solid body. We are able to observe that under adequate effective temperature and particle concentration conditions, crystalline pattern formation occurs. We first describe the system and discuss the experiments we conducted at several cooling rates to explore the effect of effective temperature and particle concentration on the resulting pattern formation.

Results
Conclusion
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