Abstract

Large-Eddy Simulations (LESs) and experiments were employed to study the influence of water depth on the hydrodynamics in the wake of a conical island for emergent, shallow, and deeply submerged conditions. The Reynolds numbers based on the island’s base diameter for these conditions range from 6500 to 8125. LES results from the two shallower conditions were validated against experimental measurements from an open channel flume and captured the characteristic flow structures around the cone, including the attached recirculation region, vortex shedding, and separated shear layers. The wake was impacted by the transition from emergent to shallow submerged flow conditions with more subtle changes in time-averaged velocity and instantaneous flow structures when the submergence increases further. Despite differences in the breakdown of the separated shear layers, vortex shedding, and the upward flow region on the leeward face (once the cone’s apex is submerged), similar flow structures to cylinder flow were observed. These include an arch vortex tilted in the downstream direction and von Karman vortices in the far-wake. Spectra of velocity time series and the drag coefficient indicated that the vortex shedding was constrained by the overtopping flow layer, and thus the shedding frequency decreased as the cone’s apex became submerged. Finally, the generalised flow structures in the wake of a submerged conical body are outlined.

Highlights

  • In open channel flows, most turbulent shallow wakes are generated by three-dimensional (3D) obstacles, such as boulders, bridge piers, islands, screens, and plants

  • Large-eddy simulations (LESs) and experiments have been used to investigate the wake generated by a conical island for three levels of submergence: surface-piercing (H h = 0.96), shallow submergence (H h = 1.24), and deeply submerged (H h = 1.92) conditions

  • The high-resolution Large-Eddy Simulations (LESs) allowed for the identification of key instantaneous flow structures, reproducing well the time-averaged flow properties observed in the experiments

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Summary

INTRODUCTION

Most turbulent shallow wakes are generated by three-dimensional (3D) obstacles, such as boulders, bridge piers, islands, screens, and plants. Streamwise tip vortices formed off the freeend of the obstacle have been observed for a variety of object shapes and profiles.5,8–11 These vortices shift downwards with the downwash flow, and for the case of cylinders with smaller aspect ratios, they occupy a greater proportion of the water column and dominate the turbulence structures, which prevents the development of von Karman vortex shedding.. Large-Eddy Simulations (LESs) demonstrated that the tip vortices and recirculation bubbles at a cylinder’s free-end are not significantly affected by the presence of a vertical plate attached to the downstream side of the cylinder and only the arch vortex and horseshoe vortex were affected.. The model is first validated against experimental data for both emergent and shallow submerged conditions and applied to a deeper submergence case to better understand how conical island submergence impacts time-averaged flow properties and instantaneous flow structures in its wake

EXPERIMENTAL SETUP
Numerical framework
Computational setup
RESULTS AND DISCUSSION
Mesh sensitivity
Time-averaged velocity field
Instantaneous flow structures
Second-order statistics
Deeper submergence case
Hydrodynamic forces and far-wake characterisation
CONCLUSIONS
Methods
Full Text
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