Publication | Open Access
A mechanism for the generation of wave‐driven rhythmic patterns in the surf zone
169
Citations
29
References
2000
Year
Ocean DynamicsEngineeringSurface WaveShallow Water HydrodynamicsOceanographyCoastal ProcessCoastal HydrodynamicsWave MotionTopographic PerturbationsEarth ScienceNonlinear Ocean WavesNearshore ProcessNearshore ProcessesWave AnalysisWave DynamicsOcean Internal WaveOcean Wave MechanicsWave Radiation StressCoastal ProcessesSediment TransportPattern FormationMorphodynamicsCivil EngineeringGeomechanicsBeach DynamicSurf ZoneWave‐driven Rhythmic Patterns
Topographic irregularities generate excess wave‑radiation‑stress gradients that drive a steady circulation, which in turn creates sediment‑transport patterns that can reinforce bottom disturbances and promote large‑scale bed‑form growth. The study investigates how topographic irregularities couple with wave‑driven mean water motion by solving a linearized stability problem for a plane beach under normal wave incidence. The authors analyze two scenarios: one with a fixed breaking line and another where water‑depth perturbations shift the breaker line. In the fixed‑breaker case, the topography is unstable to a giant cusp pattern of transverse bars spanning the surf zone and a crescentic pattern of alternating shoals and pools, whereas allowing the breaker line to shift suppresses the giant cusp growth but leaves the crescentic pattern largely unaffected.
The coupling between topographic irregularities and wave‐driven mean water motion in the surf zone is examined. This coupling occurs because the topographic perturbations produce excess gradients in the wave radiation stress that cause a steady circulation. This circulation, in turn, creates a sediment transport pattern that can reinforce the bottom disturbance and may thereby lead to the growth of large‐scale bed forms. To investigate this coupling mechanism, the linearized stability problem with an originally plane sloping beach and normal wave incidence is solved in two different cases. First, the breaking line is considered to be fixed, and second, the perturbations in water depth that produce a displacement of the breaker line are accounted for. The first case shows that the basic topography can be unstable with respect to two different modes: a giant cusp pattern with shore‐attached transverse bars that extend across the whole surf zone and a crescentic pattern with alternate shoals and pools at both sides of the breaking line showing a mirroring effect. In the second case, the varying breaker line may have a strong influence on the circulation. This is clear for the giant cusp topography whose growth is totally inhibited. In contrast, the morphology and the growth of the crescentic pattern remains almost unchanged.
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