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Kadanoff Sand Pile Model, Avalanche Structure and Wave Shape

Author

Listed:
  • Kévin Perrot

    (LIP - Laboratoire de l'Informatique du Parallélisme - ENS de Lyon - École normale supérieure de Lyon - UCBL - Université Claude Bernard Lyon 1 - Université de Lyon - Inria - Institut National de Recherche en Informatique et en Automatique - Université de Lyon - CNRS - Centre National de la Recherche Scientifique, Laboratoire d'Informatique, Signaux, et Systèmes de Sophia-Antipolis (I3S) / Equipe MC3 - Laboratoire I3S - MDSC - Modèles Discrets pour les Systèmes Complexes - I3S - Laboratoire d'Informatique, Signaux, et Systèmes de Sophia Antipolis - UNS - Université Nice Sophia Antipolis (1965 - 2019) - CNRS - Centre National de la Recherche Scientifique - UniCA - Université Côte d'Azur)

  • Éric Rémila

    (LIP - Laboratoire de l'Informatique du Parallélisme - ENS de Lyon - École normale supérieure de Lyon - UCBL - Université Claude Bernard Lyon 1 - Université de Lyon - Inria - Institut National de Recherche en Informatique et en Automatique - Université de Lyon - CNRS - Centre National de la Recherche Scientifique, GATE Lyon Saint-Étienne - Groupe d'Analyse et de Théorie Economique Lyon - Saint-Etienne - ENS de Lyon - École normale supérieure de Lyon - UL2 - Université Lumière - Lyon 2 - UCBL - Université Claude Bernard Lyon 1 - Université de Lyon - UJM - Université Jean Monnet - Saint-Étienne - CNRS - Centre National de la Recherche Scientifique)

Abstract

Sand pile models are dynamical systems describing the evolution from NN stacked grains to a stable configuration. It uses local rules to depict grain moves and iterate it until reaching a fixed configuration from which no rule can be applied. Physicists L. Kadanoff et al. inspire KSPM, extending the well known Sand Pile Model (SPM). In KSPM(DD), we start from a pile of NN stacked grains and apply the rule: D−1D−1 grains can fall from column ii onto columns i+1,i+2,...,i+D−1i+1,i+2,...,i+D−1 if the difference of height between columns ii and i+1i+1 is greater or equal to DD. Toward the study of fixed points (stable configurations on which no grain can move) obtained from NN stacked grains, we propose an iterative study of KSPM evolution consisting in the repeated addition of one grain on a heap of sand, triggering an avalanche at each iteration. We develop a formal background for the study of avalanches, resumed in a finite state word transducer, and explain how this transducer may be used to predict the form of fixed points. Further precise developments provide a plain formula for fixed points of KSPM(3), showing the emergence of a wavy shape.

Suggested Citation

  • Kévin Perrot & Éric Rémila, 2013. "Kadanoff Sand Pile Model, Avalanche Structure and Wave Shape," Post-Print halshs-00949239, HAL.
  • Handle: RePEc:hal:journl:halshs-00949239
    DOI: 10.1016/j.tcs.2013.01.033
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    Cited by:

    1. Kévin Perrot & Eric Rémila, 2017. "Strong Emergence of Wave Patterns on Kadanoff Sandpiles," Post-Print halshs-01417254, HAL.

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