Difference between revisions of "Perturbation Spreading in Many-Particle Systems: A Random Walk Approach"

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(Summary)
(Summary)
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The authors knew that a propagation would travel through the material at approximately a finite  velocity. Typical diffusion equations, however, imply infinite propagation speeds; the authors consequently knew this would not accurately describe their system's behavior. Consequently, the authors decided to model the perturbation kinetics by treating the particles as if they were undergoing a random walk.
 
The authors knew that a propagation would travel through the material at approximately a finite  velocity. Typical diffusion equations, however, imply infinite propagation speeds; the authors consequently knew this would not accurately describe their system's behavior. Consequently, the authors decided to model the perturbation kinetics by treating the particles as if they were undergoing a random walk.
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Specifically, the authors applied the "continuous-time random walk formalism" (CTRW) to the particles. This implied that a particle would travel at a constant speed <math>v_o</math> and at turning points would randomly change the direction of its motion. The time between collisions was drawn from a Probability Density Function (PDF) described by
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<math>P(t)\propto(\frac{\tau}{\tau_o})^{-\gamma-1}</math>
  
 
==Discussion==
 
==Discussion==
  
 
==References==
 
==References==

Revision as of 21:54, 18 September 2012

Original entry by Bryan Weinstein, Fall 2012

General Information

Authors: V. Zaburdaev, S. Denisov, and P. Hanggi

Keywords:

Summary

The authors of this paper examine the propagation dynamics of a perturbation traveling through a non-dissipative medium (energy is conserved and not lost due to friction). They modeled the medium as a collection of many interacting particles. As energy was conserved, they were able to apply Hamiltonian dynamics to analyze the system.

The authors knew that a propagation would travel through the material at approximately a finite velocity. Typical diffusion equations, however, imply infinite propagation speeds; the authors consequently knew this would not accurately describe their system's behavior. Consequently, the authors decided to model the perturbation kinetics by treating the particles as if they were undergoing a random walk.

Specifically, the authors applied the "continuous-time random walk formalism" (CTRW) to the particles. This implied that a particle would travel at a constant speed <math>v_o</math> and at turning points would randomly change the direction of its motion. The time between collisions was drawn from a Probability Density Function (PDF) described by

<math>P(t)\propto(\frac{\tau}{\tau_o})^{-\gamma-1}</math>

Discussion

References