Confinement effects in shallow-water jets
AM Shinneeb, R Balachandar… - Journal of Hydraulic …, 2011 - ascelibrary.org
AM Shinneeb, R Balachandar, JD Bugg
Journal of Hydraulic Engineering, 2011•ascelibrary.orgThis paper documents measurements of the mean velocity field and turbulence statistics of
an isothermal, round jet entering a shallow layer of water. The lower boundary of the jet was
a solid wall and the upper boundary a free surface. The jet axis was midway between the
solid wall and the free surface in all cases. Experiments were performed at a Reynolds
number of 22,500 for water layer depths 15, 10, and 5 times the jet exit diameter (9 mm).
Particle image velocimetry measurements were made on vertical and horizontal planes …
an isothermal, round jet entering a shallow layer of water. The lower boundary of the jet was
a solid wall and the upper boundary a free surface. The jet axis was midway between the
solid wall and the free surface in all cases. Experiments were performed at a Reynolds
number of 22,500 for water layer depths 15, 10, and 5 times the jet exit diameter (9 mm).
Particle image velocimetry measurements were made on vertical and horizontal planes …
This paper documents measurements of the mean velocity field and turbulence statistics of an isothermal, round jet entering a shallow layer of water. The lower boundary of the jet was a solid wall and the upper boundary a free surface. The jet axis was midway between the solid wall and the free surface in all cases. Experiments were performed at a Reynolds number of 22,500 for water layer depths 15, 10, and 5 times the jet exit diameter (9 mm). Particle image velocimetry measurements were made on vertical and horizontal planes—both containing the axis of the jet. The measurements were taken from 10 to 80 jet diameters downstream. Results showed that, for the highly confined cases at downstream locations, the axial velocity was quite uniform over the depth, with a mild peak below the jet axis. In the horizontal plane, the velocity profiles were slightly narrower than the free jet profile, but in the vertical plane, they were wider. The mean vertical velocity profiles showed that entrainment was suppressed in the vertical direction. At the same time, the lateral velocity profiles indicate that fluid flows from the sides toward the jet centerline. For the shallow cases, the mean vertical velocity becomes negative over most of the depth at downstream locations, indicating that this inflow from the sides is directed downward toward the solid wall. The relative turbulence intensity results were suppressed in the axial and vertical directions and mildly enhanced in the lateral direction. As well, the Reynolds shear stress in the vertical plane was significantly reduced by the vertical confinement, while in the horizontal plane it was only slightly affected by the confinement.
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