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Phys. Rev. Lett. 98, 084502 (2007) [4 pages]

Heavy Particle Concentration in Turbulence at Dissipative and Inertial Scales

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J. Bec1, L. Biferale2, M. Cencini3, A. Lanotte4, S. Musacchio5, and F. Toschi6
1CNRS UMR6202, Observatoire de la Côte d’Azur, BP4229, 06304 Nice Cedex 4, France
2Dipartimento di Fisica and INFN, Università “Tor Vergata,” Via Ricerca Scientifica 1, 00133 Roma, Italy
3INFM-CNR, SMC Department of Physics, Università “La Sapienza,” Piazzale Aldo Moro 2, 00185 Roma, Italy, and CNR-ISC, Via dei Taurini 19, 00185 Roma, Italy
4CNR-ISAC and INFN, Sezione di Lecce, Strada Provinciale Lecce-Monteroni, 73100 Lecce, Italy
5Weizmann Institute of Science, Department of Physics of Complex Systems, 76100 Rehovot, Israel
6CNR-IAC, Viale del Policlinico 137, 00161 Roma, Italy, and INFN, Sezione di Ferrara, Via G. Saragat 1, 44100 Ferrara, Italy

Received 18 August 2006; published 21 February 2007

Spatial distributions of heavy particles suspended in an incompressible isotropic and homogeneous turbulent flow are investigated by means of high resolution direct numerical simulations. In the dissipative range, it is shown that particles form fractal clusters with properties independent of the Reynolds number. Clustering is there optimal when the particle response time is of the order of the Kolmogorov time scale . In the inertial range, the particle distribution is no longer scale invariant. It is, however, shown that deviations from uniformity depend on a rescaled contraction rate, which is different from the local Stokes number given by dimensional analysis. Particle distribution is characterized by voids spanning all scales of the turbulent flow; their signature in the coarse-grained mass probability distribution is an algebraic behavior at small densities.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.98.084502
DOI:
10.1103/PhysRevLett.98.084502
PACS:
47.27.−i, 47.10.−g