Abstract
k − − ε models for the analysis of transport of solid particles in gas flows are reported in a number of papers: Reeks (1991, 1992), Simonin (1991), Sommerfeld (1992) and Wolkov et al. (1994), and the references given therein, are good places to start. The common feature of these works is the assumption of convection and diffusion of the specific turbulent kinetic energy and its dissipation in the continuous phase. To consider the influence of the discrete phase, two approaches are generally used:
(a) No feedback of the dispersed phase on the continuum turbulence, commonly named one-way coupling.
(b) The feedback of the dispersed phase on the continuum turbulence is taken into account. This approach is named two-way coupling.
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Kolev, N.I. (2011). Particle-eddy interactions. In: Multiphase Flow Dynamics 4. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-20749-5_6
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DOI: https://doi.org/10.1007/978-3-642-20749-5_6
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