Modeling and analyzing observed transverse sand bars in the surf zone
Author(s) -
Ribas F.,
Swart H. E.,
Calvete D.,
Falqués A.
Publication year - 2012
Publication title -
journal of geophysical research: earth surface
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/2011jf002158
Subject(s) - shoal , surf zone , geology , transverse plane , submarine pipeline , sediment transport , wavelength , current (fluid) , crest , bar (unit) , turbulence , bedform , longshore drift , bed load , mechanics , geotechnical engineering , sediment , geomorphology , physics , oceanography , optics , structural engineering , engineering
A morphodynamic model has been applied to explain the characteristics of transverse sandbars observed in the inner surf zone of open beaches. The model describes the feedback between waves, rollers, depth‐averaged currents and bed evolution, so that self‐organized processes can develop. The modeled bar characteristics, i.e. wavelength (30–70 m), crest orientation (up‐current) and the e‐folding growth time (about 12 hr) are in good agreement with those of observed transverse bars at Noordwijk beach, the Netherlands, but modeled migration speeds (tens of meters per day), turn out to be a factor 2 larger than those observed. The wavelength increases with the distance between the shoreline and the peak of the longshore current and the migration speed is correlated with the maximum longshore current. The model also explains why transverse bar formation at Noordwijk occurs for obliquely incident waves of intermediate heights. Realistic positive feedback leading to formation of up‐current oriented bars like those observed is only obtained if a term related to the turbulence sediment resuspension created by the rollers is included in the transport formula. In that case, the depth‐averaged sediment concentration decreases seaward across the inner surf zone, enhancing the convergence of sediment transport in the offshore directed flow perturbations that occur over the up‐current bars. This offshore current deflection is mainly caused by frictional torques, but the roller radiation stresses also play an important role.
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