SIMULATOR. Jentsje W. van der Meer1, Gosse Jan Steendam2, Govertine de Raat3 and ..... Wave overtopping erosion tests at Groningen sea dyke. ComCoast,.
FREEBOARD. David K. Jones1, Qingping Zou2, Dominic E. Reeve3 .... H. R. Hg q. Q ξ ξ α. 98.1 exp. 051.0 tan . . 3 for p ξ < 2.0. (5)....... â. = =.
GRASS COVERED SLOPES OF DIKES. Gosse Jan ... stability of grass covered dike slopes. These tests .... All tests were filmed and measurements of damages.
The Large Wave Flume (GWK) in Hannover has a length of about 300 m, a width of 5 m ..... The highest force peak is obtained with Fint = 7.6kN/m for this test. It.
The calibration led to a procedure to create the correct steering .... Hughes and Nadal (2009) have performed overtopping tests where the water level was even ...
Extreme wave heights and storm surges are often generated by high wind speeds in large areas ... Low-crested structures are obstacles for waves and will dissipate energy. The result is a ... with gentle outer slope and various crest widths.
3 Van der Meer Consulting, P.O. Box 423, 8440 AK Heerenveen, Netherlands .... to 500 l/m) there is no difference between velocity at ground level and the top of.
2 Flanders Hydraulics Research, Berchemlei 115, B-2140, Antwerp, Belgium, ... The river Schelde stretches from the Dutch-Belgian border all the way to the city.
Sep 14, 2017 - College of Engineering, Swansea University, Fabian Way, Swansea SA1 ... high tide at Aberystwyth, which in addition to a storm surge and ...
Jun 20, 2016 - Myron van Damme. Delft University .... Hunt (1959) related the run-up height of an ... Battjes (1974) adapted the Hunt run-up formula to irregular.
the first step in a project to extend the model to encompass vertical structures. Use is made of .... Rmax > Rc/γf , there is no overtopping apart from wind-blown spray. Figure 1 shows ..... Wave overtopping formula for gentle slopes incorporating .
Soliman (2003) investigated the influences of seawall slope, wave type and crest freeboard on overtopping discharges of irregular wave based on the RANS ...
to measure the velocity of a small ship and exists of a small paddle wheel in a frame. Every turn around of ...... a bit quicker and easier to read. 6.5 Conclusion ...
In the current paper, only smooth dike slope (no roughness elements) and ..... An increased bullnose angle ε reduces the amount of overtopping, but increases .... and 1.2m high storm wall in prototype, being an optimal solution for the Belgian ...
(1999); the TAW Technical Report on Wave run up and wave overtopping at dikes by van der Meer ...... E+01. 1.E+02. 1.E+03. Overtopping discharge q [l/s/m]. M a ximu m vo lume ...... 25th Int. Conf. on Coastal Engng. Orlando. pp 2216â2229.
readily available (e.g., desktop or laptop computers), thus giving engineers the ability to conduct multiple ..... slowest and fastest travelling wavespeeds (msâ1). T.
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Luc VAN DAMME2, Flemming SCHLUTTER3, John DE RONDE4 .... Owen (1980) relates a dimensionless freeboard to a dimensionless discharge by an.
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Wave structure interaction during hurricane ivan simulated by a two-phase flow model. Coastal Hazards, pages 33â44, 2013. doi: 10.1061/9780784412664.004.
crest of a sea wall is set too low then there are potential problems with structural safety and flooding from wave overtopping. Hence, it is important to strike the ...
the overtopping prediction formula published in the EurOtop (2007) manual. With these ...... suction of water has not yet started), and a cool-down phase of about 2 s ...... steepness sop = 0.04) are similar to the B values of the analysed datasets.
connects the small clay aggregates and prevents them fi-om being washed out, ... For uniform fiow and hydraulic smooth conditions, Nezu (1977) found CTâ{ ... linear distributed ko = 1.65(M*)1 Since /
CREST CAISSON BREAKWATERS. Giovanni Cuomo1, Andrea Polidoro1,2, Elettra Pasquini3, John Alderson1, David. Robinson1, William Allsop1 and Scott ...
WAVE LOADING, OVERTOPPING AND TRANSMISSION OF LOW CREST CAISSON BREAKWATERS Giovanni Cuomo1, Andrea Polidoro1,2, Elettra Pasquini3, John Alderson1, David Robinson1, William Allsop1 and Scott Dunn1 Recent LNG projects have pointed out the efficiency of low crested caissons breakwaters in providing shelter from waves to LNG terminals during frequent conditions whilst allowing for wave overtopping / transmission during most severe storms, reducing the design loads and therefore the overall cost of the breakwater. Unfortunately, little is known on hydrodynamic behaviour and loading of low crested structures heavily overtopped by long waves and use of existing design codes generally leads to over-design and excessive construction costs. Bearing this in mind, both physical and numerical models have been successfully applied to investigate wave-structure interaction problems and in particular to improve accuracy and increase confidence in the estimations of wave loading, wave overtopping and transmission over low crested structures. Tentative semi-empirical formulas are presented for wave overtopping and wave transmission based on new experimental data.
INTRODUCTION
Many recent LNG projects have required dedicated terminals, often sheltered by a dedicated breakwater. As shelter for loading / offloading operations is only required over relatively non-extreme wave conditions, the breakwater can be tuned to limit wave transmission during frequent conditions whilst allowing for wave overtopping / transmission during most severe storms. This reduces design loads on the caisson, and therefore the overall cost of the breakwater. Given the scarcity of details provided in design codes, a series of numerical and physical model studies have been completed with the aim of developing new guidance on: • Influence of crest width on wave transmission • Reflection coefficients for submerged crest structures • Vertical uplift / downward pressures during significant overtopping events • Effect of reducing crest level and caisson width on: o Loading / stability o Wave transmission Previous work
Wave transmission over caisson breakwater was firstly investigated by Goda (1969) who derived a prediction method based on measurements from physical model tests performed using regular waves. Goda’s original work was later extended by Takahashi (1996) who suggests that the above formulation is still 1
HR Wallingford – Howbery Park, Wallingford, Oxfordshire OX10 8BA, UK Dipartimento di Ingegneria Idraulica, Geotecnica ed Ambientale (DIGA) Facoltà di Ingegneria - Università degli Studi di Napoli Federico II 3 Dipartimento di Ingegneria Civile, Ambientale e dei Materiali (DICAM) Facolta di Ingegneria - Alma Mater Studiorum Università di Bologna 2
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2 applicable to random waves when using Hs as input. For the irregular wave case, calculated from: 0.5 2 2 0.251 − sin (π / 2α ) Rc + β + 0.011 − d H h s Ctr = d 0.11 − h