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EurOCEAN 2000 - Vlaams Instituut voor de Zee

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Both the <strong>Zee</strong>brugge and the Petten sites are<br />

accurately mo<strong>de</strong>lled and tested in 5 different<br />

laboratories. Mo<strong>de</strong>l tests are carried out in 2D<br />

wave flumes (Flan<strong>de</strong>rs Hydraulics, Delft<br />

Hydraulics and Universidad Politecnica <strong>de</strong><br />

Valencia) and in 3D wave tanks (Aalborg<br />

University and University College Cork) to cover<br />

a whole range of parametric tests and the<br />

reproduction of measured storms. The scale of<br />

the mo<strong>de</strong>ls varies between 1:30 and 1:40. In<br />

or<strong>de</strong>r to mo<strong>de</strong>l the flow in the core of the<br />

breakwater properly a special scaling method has<br />

been chosen for scaling the core material<br />

(Burcharth et al. (1999)), resulting into coarser<br />

Fig. 4: UG-step gauge<br />

core material than the overall scale. The <strong>Zee</strong>brugge mo<strong>de</strong>l is also tested in a combined wave<br />

flume and wind tunnel to study the influence of wind on run-up, overtopping and spray.<br />

Failure of a seawall is often initiated by damage to the crest. When waves overtop the structure,<br />

the downrushing water may damage the landward slope of a dike. This can lead to the total<br />

failure of the structure.<br />

Therefore the crest stability is studied in a wave flume. A series of mo<strong>de</strong>l tests on wave<br />

overtopping and wave run-up is carried out to investigate wave overtopping rates, overtopping<br />

velocities and water layer thicknesses for different seaward (1:6, 1:4 and 1:3) and landward<br />

slopes. Tests are performed for regular and irregular waves, for different freeboards and water<br />

<strong>de</strong>pths,… in or<strong>de</strong>r to test a wi<strong>de</strong> range of parameters. The results of this investigation will help<br />

in a better assessment of the crest stability of overtopped structures.<br />

•<br />

• DISCUSSION OF RESULTS<br />

Analysis of the available <strong>Zee</strong>brugge data<br />

reveals many points of interest. The<br />

Ru 2%<br />

dimensionless run-up value seems<br />

H mo<br />

to be <strong>de</strong>pen<strong>de</strong>nt on the water level:<br />

Ru 2%<br />

values increase when water <strong>de</strong>pth<br />

H mo<br />

<strong>de</strong>creases. Ru is <strong>de</strong>fined as the difference<br />

between wave run-up level and mean water<br />

level. The run-up which is excee<strong>de</strong>d by 2 %<br />

of the run-up events is called Ru2%. Hmo is<br />

the significant wave height, based on<br />

spectral analysis. When time series of<br />

492<br />

Ru 2%/H mo [-]<br />

3<br />

2<br />

1<br />

0<br />

-1<br />

-2<br />

0 1 2 3 4 5<br />

Rd 2%/H mo [-]<br />

ξ m [-]<br />

<strong>Zee</strong>brugge small scale results (Murphy et al. (1996))<br />

<strong>Zee</strong>brugge prototype results<br />

Fig. 5: Comparison between prototype<br />

and scale mo<strong>de</strong>l wave run-up results

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