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EurOCEAN 2000 - Vlaams Instituut voor de Zee

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transport rate has been measured for normal and enhanced turbulence levels over flat and<br />

rippled sand beds. Two further practical aspects have been consi<strong>de</strong>red; (1) given the magnitu<strong>de</strong><br />

of the extra turbulence, can the sediment transport rate be calculated?, and (2) can the<br />

magnitu<strong>de</strong> of the extra turbulence be predicted without recourse to in-<strong>de</strong>pth investigations? To<br />

address these issues a baseline study of the <strong>de</strong>tailed processes of suspen<strong>de</strong>d sediment transport<br />

in a turbulent tidal flow has been completed. To extend these data, the results from numerical<br />

simulations have been applied to quantify the effect of enhanced turbulence levels on<br />

suspen<strong>de</strong>d sediment transport (1DV mo<strong>de</strong>l), and bedload (CFD co<strong>de</strong>). The effects of breaking<br />

waves, turbulence and vortex shedding on bed stability and scour have also been assessed<br />

(Simons, 1999), and an analytical approach for predicting sediment transport proposes. The<br />

data from the above studies will be input to the project database, and the key results will<br />

provi<strong>de</strong> input to the <strong>de</strong>sign gui<strong>de</strong>lines. The new findings will be collated with existing<br />

available information when formulating the gui<strong>de</strong>lines (e.g. Whitehouse, 1998).<br />

SEDIMENT BEHAVIOUR CLOSE TO THE STRUCTURE AND<br />

SCOUR (TASK 2)<br />

The work in this part of the project (Task 2, led by SINTEF ) concentrates on the processes<br />

associated with the sediment, which is closely related to the wave-generated pore pressure in<br />

the sediment bed. This task is sub-divi<strong>de</strong>d into six topics:<br />

TOPIC 2.1. WAVE-GENERATED PORE PRESSURE AND SCOUR AROUND<br />

BREAKWATER ELEMENTS. UOX has carried out field measurements on wave generated<br />

pore pressures in a sand seabed. A typical element of a breakwater (a rubble mound stone) is<br />

simulated with a truncated cylin<strong>de</strong>r placed on the seabed with the axis vertical. Wave-induced<br />

pressures are measured on the cylin<strong>de</strong>r as well as in the seabed. There is also an altimeter and<br />

an inclinometer to monitor the scour at the cylin<strong>de</strong>r as well as the tilt of the cylin<strong>de</strong>r. UOX has<br />

actually achieved four field <strong>de</strong>ployments of an instrumented cylin<strong>de</strong>r. Due to experimental<br />

problems, the two first were unsuccessful, but the two following ones successfully produced<br />

data. Consi<strong>de</strong>rable erosion and consequent tilting of the mo<strong>de</strong>l breakwater element have been<br />

observed in all the <strong>de</strong>ployments. The data is being analysed.<br />

TOPIC 2.2. NON-LINEAR MODELLING OF WAVE INDUCED PORE PRESSURES.<br />

SINTEF has mo<strong>de</strong>lled pore pressure and effective stresses using non-linear material mo<strong>de</strong>ls.<br />

The non-linear material is a swelling soil mo<strong>de</strong>l.<br />

Based on numerical results, the following conclusions have drawn: (1) Elasto-plastic soil<br />

behaviour reduces gradients out of the seabed when critical gradients are reached. (2) Critical<br />

gradients out of bed can be reached with a small content of gas in the pore fluid. (3) Shallow<br />

water non-linear breaking waves gives lower gradients out of bed than "linear non-breaking"<br />

waves of similar height and period in the same water <strong>de</strong>pth. See also Ilstad et al. (<strong>2000</strong>).<br />

TOPIC 2.3. WAVE BOTTOM PRESSURES AND WAVE KINEMATICS IN THE SURF<br />

ZONE. NTNU and SINTEF have obtained spatial and temporal variations of the dynamic<br />

bottom pressures and the wave kinematics in the vicinity of the wave breaking point in shallow<br />

water. Different numerical schemes have been tested to calculate the surface elevation, wave<br />

kinematics and bottom pressures FIRAM (Finite Element Reynolds Average Mo<strong>de</strong>l), VOF<br />

(Volume Of Fluid) and COBRAS (Cornell Breaking - Wave And Structures). The latter mo<strong>de</strong>l<br />

seems so far to give reasonable agreement with measurements. See also: Arntsen et al. (<strong>2000</strong>).<br />

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