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Near field vorticity distributions from a sharp-edged rectangular jet
•Axial mean vorticity equation terms are calculated from experimental data.•Appearance of ridges, dumbbell shape and saddleback velocity profiles is highlighted.•Explanations are provided using terms from the vorticity equation. Experimental results on the near field development of a free rectangula...
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Published in: | The International journal of heat and fluid flow 2015-02, Vol.51, p.383-394 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | •Axial mean vorticity equation terms are calculated from experimental data.•Appearance of ridges, dumbbell shape and saddleback velocity profiles is highlighted.•Explanations are provided using terms from the vorticity equation.
Experimental results on the near field development of a free rectangular jet with aspect ratio 10 are presented. The jet issues from a sharp-edged orifice attached to a rectangular settling chamber at Reh∼23,000, based on slot width, h. Measurements on cross plane grids were obtained with a two-component hot wire anemometry probe, which provided information on the three dimensional characteristics of the flow field. Two key features of this type of jet are mean axial velocity profiles presenting two off axis peaks, commonly mentioned as saddleback profiles, and a predominant dumbbell shape as described by, for example, a contour of the axial mean velocity. The saddleback shape is found to be significantly influenced by the vorticity distribution in the transverse plane of the jet, while the dumbbell is traced to two terms in the axial mean vorticity transport equation that diffuse fluid from the centre of the jet towards its periphery. At the farthest location where measurements were taken, 30 slot widths from the jet exit, the flow field resembles that of an axisymmetric jet. |
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ISSN: | 0142-727X 1879-2278 |
DOI: | 10.1016/j.ijheatfluidflow.2014.10.002 |