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Random packings of frictionless particles
Corey S O'Hern1, Stephen A Langer, Andrea J Liu
1Department of Chemistry and Biochemistry, UCLA, Los Angeles, California 90095-1569, USA.
Physical Review Letters
|February 28, 2002
Summary
Randomly packed frictionless particles jam at a critical packing fraction. As system size increases, this jamming threshold distribution narrows, revealing non-self-averaging behavior and exponential force decay.
Area of Science:
- Physics
- Materials Science
- Statistical Mechanics
Background:
- Understanding the behavior of granular materials and particle packings is crucial in various scientific fields.
- The concept of jamming, where disordered systems transition to a solid-like state, is a key phenomenon in condensed matter physics.
Purpose of the Study:
- To investigate the jamming threshold and associated properties of frictionless particle packings at zero temperature.
- To analyze the impact of system size on the distribution of jamming thresholds and interparticle forces.
Main Methods:
- Numerical simulations of random packings of frictionless particles were performed.
- The study focused on systems at zero temperature (T = 0).
- Analysis included the calculation of packing fraction, pressure, static shear modulus, and force distributions.
Main Results:
- The packing fraction at which pressure becomes nonzero was found to be identical to the jamming threshold (where static shear modulus becomes nonzero).
- The distribution of threshold packing fractions narrows as system size increases, approaching random close packing.
- Absence of self-averaging within the peak of the threshold distribution leads to an exponential decay in interparticle force distribution.
Conclusions:
- The jamming transition in frictionless particle systems is characterized by a unique packing fraction where both pressure and shear modulus emerge.
- System size plays a critical role in narrowing the jamming threshold distribution and approaching a universal packing fraction.
- Non-self-averaging behavior at the jamming threshold dictates the statistical distribution of forces between particles.