4.5 Article

Modulation of homogeneous turbulence seeded with finite size bubbles or particles

Journal

INTERNATIONAL JOURNAL OF MULTIPHASE FLOW
Volume 36, Issue 3, Pages 221-233

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.ijmultiphaseflow.2009.11.001

Keywords

Dispersed two-phase flow; Homogeneous turbulence; Direct numerical simulation; Particle suspensions

Categories

Funding

  1. Arctic Region Supercomputing Center at the University of Alaska Fairbanks
  2. Department of Defence High Performance Computing Modernization Program
  3. DARPA
  4. CNRS [3419]

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The dynamics of homogeneous, isotropic turbulence seeded with finite sized particles or bubbles is investigated in a series of numerical simulations. using the force-coupling method for the particle phase and low wavenumber forcing of the flow to sustain the turbulence Results are given oil the modulation of the turbulence due to massless bubbles, neutrally buoyant particles and inertial particles of specific density 1 4 at volumetric concentrations of 6%. Buoyancy forces due to gravity are excluded to emphasize finite size and inertial effects for the bubbles or particles and their interactions with the turbulence Besides observing the classical entrapment of bubbles and the expulsion of inertial particles by vortex structures, we analyze the Lagrangian statistics for the velocity and acceleration of the dispersed phase. The turbulent fluctuations are damped at mid-range wavenumbers by the bubbles or particles while the small-scale kinetic energy is significantly enhanced. Unexpectedly, the modulation of turbulence depends only slightly on the dispersion characteristics (bubble entrapment in vortices or inertial sweeping of the solid particles) but is closely related to the stresslet component (finite size effect) of the flow disturbances The pivoting wavenumber characterizing the transition from damped to enhanced energy content is shown to vary with the size of the bubbles or particles. The spectrum for the energy transfer by the particle phase is examined and the possibility of representing this, at large scales, through an additional effective viscosity is discussed. (C) 2009 Elsevier Ltd. All rights reserved

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