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Modeling Wave Transformation Over An Artificial Reef (Page 1 of 7)
Introduction: |
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Waves and Wave Modeling: REF/DIF1 is representative of a new group of water wave models that have significantly improved accuracy in comparison to previous models. Until recently, only very approximate models existed which relied on ray tracing techniques and excluded diffraction. These models had difficulties modeling waves propagation over complex bathymetries. REF/DIF1 is a weakly non-linear combined refraction and diffraction model that models waves on a uniform grid, thus avoiding many of the shortcomings in ray tracing techniques (Kirby and Dalrymple, 1994). Some explanation of wave propagation and transformation as waves approach the shore will clarify the modeling procedure. Most ocean waves are generated by winds offshore. The size of the waves is dependent on three factors: wind speed, the duration of the wind, and the fetch or distance over which the wind blows (Denny, 1988). As this wind-generated chaotic sea moves away from the source their character changes. The waves organize into swells and tend to propagate in groups and their shape becomes sinusoidal. Because of the relatively simple shape and behavior of these waves traveling in very deep water, they can be described by what is known as linear wave theory, a simple water wave description. Linear wave theory has a number of assumptions, the most important for the modeling application discussed here is that linear wave theory assumes that wave height is infinitesimal relative to water depth (Denny, 1988). As waves approach the shoreline and shoal (interact with the ocean floor) they transform dramatically in several ways. Waves can be refracted, reflected, diffracted, and they can break. Diffraction occurs as waves pass a structure (i.e. island or a jetty) and energy is propagated around the structure causing the wave to "wrap" around the structure. This "wrap around" effect is responsible for many great surfing areas located near headlands where the waves "wrap around" the headland into the shadowed area and form clean, surfable waves [See Figure 3.1]. ![]()
The result is that the offshore part of the wave front swings forward relative to the slowing part and the wave crests tend to align with the coastal contours (Bascom, 1980) [See Figure 3.2]. On an irregular coast wave crests tend to converge at the headlands and concentrate wave energy. ![]()
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