### Abstract

Original language | Undefined |
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Title of host publication | Advances in Solid State Physics 42 |

Editors | B. Kramer |

Place of Publication | New York |

Publisher | Springer |

Pages | 371-382 |

Number of pages | 12 |

ISBN (Print) | 3540429077 |

DOIs | |

Publication status | Published - 2002 |

### Publication series

Name | |
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Publisher | Springer-Verlag |

### Keywords

- METIS-211509
- IR-45134

### Cite this

*Advances in Solid State Physics 42*(pp. 371-382). New York: Springer. https://doi.org/10.1007/3-540-45618-X_29

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*Advances in Solid State Physics 42.*Springer, New York, pp. 371-382. https://doi.org/10.1007/3-540-45618-X_29

**Birth and sudden death of a granular cluster.** / van der Weele, J.P.; van der Meer, Roger M.; Lohse, Detlef.

Research output: Chapter in Book/Report/Conference proceeding › Chapter › Professional

TY - CHAP

T1 - Birth and sudden death of a granular cluster

AU - van der Weele, J.P.

AU - van der Meer, Roger M.

AU - Lohse, Detlef

N1 - Advances in Solid State Physics, 1617-5034 ; 42

PY - 2002

Y1 - 2002

N2 - Granular material is vibro-fluidized in N connected compartments. For sufficiently strong shaking the particles are statistically uniformly distributed over the compartments, but if the shaking intensity is lowered this uniform distribution gives way to a clustered state. The clustering transition is experimentally shown to be of 2nd order for N = 2 compartments and of 1st order for N ≥ 3. In particular, the latter is hysteretic, involves long-lived transient states, and exhibits a striking lack of time reversibility. In the strong shaking regime, a cluster breaks down very abruptly and in its further decay shows anomalous diffusion, with the length scale going as t 1/3 rather than the standard t 1/2. We focus upon the self-similar nature of this process. The observed phenomena are all accounted for within a flux model.

AB - Granular material is vibro-fluidized in N connected compartments. For sufficiently strong shaking the particles are statistically uniformly distributed over the compartments, but if the shaking intensity is lowered this uniform distribution gives way to a clustered state. The clustering transition is experimentally shown to be of 2nd order for N = 2 compartments and of 1st order for N ≥ 3. In particular, the latter is hysteretic, involves long-lived transient states, and exhibits a striking lack of time reversibility. In the strong shaking regime, a cluster breaks down very abruptly and in its further decay shows anomalous diffusion, with the length scale going as t 1/3 rather than the standard t 1/2. We focus upon the self-similar nature of this process. The observed phenomena are all accounted for within a flux model.

KW - METIS-211509

KW - IR-45134

U2 - 10.1007/3-540-45618-X_29

DO - 10.1007/3-540-45618-X_29

M3 - Chapter

SN - 3540429077

SP - 371

EP - 382

BT - Advances in Solid State Physics 42

A2 - Kramer, B.

PB - Springer

CY - New York

ER -