Vortex Shedding in the Near Wake of Rigid and Flexible Bluff Bodies
Kenneth Desabrais, Hamid Johari
Abstract
Kenneth Desabrais, Hamid Johari
Abstract
The velocity profiles and shedding frequencies of three axisymmetric bluff bodies consisting of a disk, a cup, and a rigid canopy model were examined in the near wake, 0.25 ≤ z/D ≤ 9.0. The measurements were conducted at a Reynolds number of 1.93 × 10 5 using a single element hot-film anemometer. The data revealed that the mean velocity deficit profiles became self-similar beyond z/D ≥ 3.0, and are identical in self-similar coordinates. However, the cup and rigid canopy models recover more quickly than the disk. At least two shedding frequencies were observed in the near wake of these axisymmetric models; one corresponding to the dominant downstream mode at a Strouhal number ≈ 0.15 and the other at low Strouhal numbers which disappears after z/D ≥ 3.0. The dominant mode appears at z/D ≥ 1.6 and persists at all locations further downstream. This mode has typically been associated with a helical mode present for axisymmetric bluff bodies with a fixed separation point. A high Strouhal number mode (≈ 0.55) seen in flexible parachute canopies does not appear to be present in the near wake of these rigid models including the rigid canopy.
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The velocity profiles and shedding frequencies of three axisymmetric bluff bodies consisting of a disk, a cup, and a rigid canopy model were examined in the near wake, 0.25 ≤ z/D ≤ 9.0. The measurements were conducted at a Reynolds number of 1.93 × 10 5 using a single element hot-film anemometer. The data revealed that the mean velocity deficit profiles became self-similar beyond z/D ≥ 3.0, and are identical in self-similar coordinates. However, the cup and rigid canopy models recover more quickly than the disk. At least two shedding frequencies were observed in the near wake of these axisymmetric models; one corresponding to the dominant downstream mode at a Strouhal number ≈ 0.15 and the other at low Strouhal numbers which disappears after z/D ≥ 3.0. The dominant mode appears at z/D ≥ 1.6 and persists at all locations further downstream. This mode has typically been associated with a helical mode present for axisymmetric bluff bodies with a fixed separation point. A high Strouhal number mode (≈ 0.55) seen in flexible parachute canopies does not appear to be present in the near wake of these rigid models including the rigid canopy.
Key concepts: Bluff, Wake, Vortex shedding, Vortex, Mechanics, Kármán vortex street, Wake turbulence, Physics