4.4 Article

Inertial effects on the dynamics of rigid heavy fibers in isotropic turbulence

Journal

PHYSICAL REVIEW FLUIDS
Volume 4, Issue 6, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevFluids.4.064301

Keywords

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Funding

  1. Edmund J. Safra Philanthropic Foundation
  2. Wolfson Family Charitable Trust
  3. Technion Fund for Promotion of Research
  4. Israel Ministry of Energy [1596/15]

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While fiber-turbulence interactions are common in industrial and environmental applications, little is known about inertial fiber dynamics in isotropic turbulence. Here, rotational and translational dynamics of rigid, heavy fibers in air isotropic turbulence were measured using two-orthogonal-view, holographic cinematography. Measurements were conducted in a turbulence chamber (Re-lambda = 115). Several batches of nylon fibers with different diameters and lengths were investigated, resulting in Stokes numbers ranging between 1.0 <= St <= 32.5, and fiber length to Kolmogorov length scale ratios ranging between 3.6 <= (L) over bar/eta(k) <= 17.3. Ratios between fiber settling velocities in turbulence and quiescent conditions, (V) over bar (2)/V-s, scaled with the ratio of the rms of air fluctuating velocities, u' and V-s, similar as for spherical particles. Fiber inertia (as indicated by St) decreased the response of the fibers to the fluctuating air velocities, and ratios of the rms values of fluctuating fiber centroid velocities and air velocities dropped from 0.96 to similar to 0.77 for the highest St and were well predicted by the model of Wang and Stock [J. Atmos. Sci. 50, 1897 (1993)]. Furthermore, with increasing St, probability density functions (PDFs) of fiber centroid velocities that were well described by a normal distribution narrowed in comparison to the those of the air velocity. PDFs of in-plane fiber rotation rates could not be described by a normal distribution. In the absence of significant length effects, fiber rotation rates were governed by St. Our results indicate that the fiber tumbling rate peaks at around St approximate to 4, most likely as a result of reduced fiber alignment with the vorticity vector compared to fibers having lower St. At the highest investigated St, decreasing tumbling rates are the result of increasingly limited response to the fluctuating flow field, well predicted by the slightly modified model proposed by Bounoua et al. [Phys. Rev. Lett. 121, 124502 (2018)].

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