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i——COMPARISON WITH PREVIOUS WORK<br />

Soulsby (1989) performed velocity and suspended sediment<br />

concentration measurements over a sandwave in the Taw estuary.<br />

The observed velocity pr<strong>of</strong>iles at the bedform crests showed<br />

similar jetting due to acceleration up the flank <strong>of</strong> the bedform<br />

as our velocity pr<strong>of</strong>iles; see figures 1 and 2. The bedforms used<br />

for our work were also similar in shape, with comparable<br />

height:length ratio <strong>of</strong> about 1:15. We thus feel confident in<br />

saying that the cloud <strong>of</strong> suspended sediment deduced by Soulsby<br />

to move downstream from a sandwave, as shown in figure 3 is the<br />

separated flow region being shed, as shown in plate 1.<br />

The reasons for the unsteadiness in the local pressure gradient<br />

around the crest may be due to surface waves excited by the<br />

bedforms or by wind, the uneven flume walls, pressure<br />

fluctuations caused by the passage <strong>of</strong> large scale structures shed<br />

from upstream crests or possibly a combination <strong>of</strong> effects.<br />

This shedding phenomenon highlights the complex nature <strong>of</strong> the<br />

system. These complications hamper fundamental understanding <strong>of</strong><br />

particle-vortex interactions, which is surely the method by which<br />

the sediment is moved from the bed into the separation cloud.<br />

It points to the serious need to pinpoint the mechanism by using<br />

single sharp crests in the absence <strong>of</strong> external forcing from the<br />

eddies shed from upstream and by surface waves. When the<br />

fundamental system is understood, its extension to the real<br />

system may be trivial in the light <strong>of</strong> our current knowledge<br />

A8-6

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