Near wake of an impulsively started disk
Author(s) -
Hamid Johari,
Keith Stein
Publication year - 2002
Publication title -
physics of fluids
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.188
H-Index - 180
eISSN - 1089-7666
pISSN - 1070-6631
DOI - 10.1063/1.1502267
Subject(s) - physics , vortex ring , vortex , wake , mechanics , vorticity , breakup , starting vortex , vortex shedding , horseshoe vortex , turbulence , classical mechanics , geometry , reynolds number , mathematics
The near wake of an impulsively started disk was studied computationally by a finite element code\udwith a Smagorinsky turbulence model. The shear layer separating from the disk lip rolled up into a\udsymmetric starting vortex ring at first. As time evolved, the vortex stretched in the downstream\uddirection and flow instabilities caused the vortex ring to become wavy eventually leading to the\udbreakup of the ring. The complete breakup and shedding of the starting vortex ring took a time of\udapproximately 14D/U, where D is the disk diameter and U is the freestream velocity. The starting\udvortex ring circulation attained a plateau of ~2.6UD at a time of about 4D/U, in good agreement\udwith the experimental findings by Balligand(2000). The radial circulation profiles are Gaussian\udduring the symmetric phase and collapse together at a time of 4D/U. Beyond this time, the vortex\udring celerity is constant and vorticity extends to the symmetry axis. The base pressure coefficient\udbecomes positive as the vortex ring moves away from the disk and remains positive until the ring\udis completely shed. The breakup of the starting vortex ring is concurrent with the appearance of an\udazimuthal pressure gradient and core flow. Following the breakup of the starting vortex ring, the\udflow became three-dimensional and settled into an open wake. The mean drag and base pressure\udcoefficients were nearly constant after a time of approximately 30D/U and matched very well\udagainst experimental data
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