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Force distributions in a triangular lattice of rigid bars
Brian P Tighe1, Joshua E S Socolar, David G Schaeffer
1Department of Physics and Center for Nonlinear and Complex Systems, Duke University, Durham, North Carolina 27708, USA.
Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|October 26, 2005
Summary
We investigated force distributions in triangular networks under stress. Under isotropic stress, forces decay superexponentially, even in diluted networks. Anisotropic stress leads to broader, exponential force tails.
Area of Science:
- Physics
- Materials Science
- Network Science
Background:
- Understanding force distribution in complex networks is crucial for material stability.
- Nontensile contact forces in granular materials and engineered structures exhibit unique behaviors.
- Network geometry significantly influences mechanical properties.
Purpose of the Study:
- To analyze the probability distribution of single-contact forces in uniformly weighted triangular networks.
- To investigate how isotropic and anisotropic stresses affect force distributions.
- To examine the impact of lattice dilution to the rigidity percolation threshold on force distributions.
Main Methods:
- Simulating uniformly weighted ensembles of force-balanced configurations.
- Applying periodic boundary conditions for isotropic compressive stress.
- Imposing anisotropic stresses on triangular lattices.
- Analyzing force distributions in both intact and diluted lattices.
Main Results:
- Under isotropic stress, single-contact force distributions exhibit superexponential decay.
- This superexponential decay is maintained in lattices diluted to the rigidity percolation threshold.
- Anisotropic stresses induce a broader tail in the force distribution, approaching exponential decay in the infinite size/anisotropy limit.
Conclusions:
- The nature of applied stress (isotropic vs. anisotropic) fundamentally alters force distribution tails in these networks.
- Lattice dilution to the rigidity percolation threshold does not change the superexponential decay under isotropic stress.
- The transition to exponential decay under anisotropic stress highlights critical behaviors at large scales and high anisotropy.