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Laboratory experiments simulating a coastal river inflow

123

Citations

28

References

2006

Year

Abstract

The dynamics of buoyant water entering a rotating basin are studied using a series of laboratory experiments designed to elucidate the alongshore transport mechanisms in river plumes. Inflowing water, which is discharged perpendicular to the tank wall, is observed to form a growing anticyclonic bulge and a coastal current downstream of the bulge. Detailed simultaneous measurements of the velocity and buoyancy fields in the plume confirm that the bulge momentum is in a gradient–wind balance and the coastal current is geostrophic. The growth of the bulge and accumulation of fluid within it coincides with a reduction in coastal current transport to approximately 50% of the inflow discharge. The bulge is characterized by a depth scale, $h$ , which is proportional to the geostrophic depth, $h_{g}$ , and two time-dependent horizontal length scales, $y_{c}$ , the displacement of the bulge centre from the wall, and $r_{b}$ , the effective radius of the bulge. These two length scales are proportional to the inertial radius, $L_{i}$ , and the local Rossby radius, $L_{b}$ , respectively. When $r_{b}\gg y_{c}$ , the bulge is held tightly to the wall, and a relatively large fraction of the inflow discharge is forced into the coastal current. For plumes with $y_{c}$ approaching $r_{b}$ , the bulge is further from the wall, and the coastal current flux is reduced. Once ${y_{c}}/{r_{b}}\,{>}\,0.7$ , the bulge separates from the wall causing flow into the coastal current to cease and the bulge to become unstable. In this state, the bulge periodically detaches from and re-attaches to the wall, resulting in pulsing transport in the coastal current. Scaling of the bulge growth based on $h_{g}$ , $L_{i}$ and $L_{b}$ predicts that it will increase as $\hbox{\it Ro}^{1/4}$ , where $\hbox{\it Ro}$ is the inflow Rossby number. The bulge growth, inferred from direct measurements of the coastal current transport, is proportional to $\hbox{\it Ro}^{0.32}$ and agrees with the predicted dependence within the experimental error.

References

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