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Civil-Comp Proceedings
ISSN 1759-3433 CCP: 94
PROCEEDINGS OF THE SEVENTH INTERNATIONAL CONFERENCE ON ENGINEERING COMPUTATIONAL TECHNOLOGY Edited by:
Paper 82
Simulation of the Shoreline Change behind a Submerged Permeable Breakwater C.P. Tsai1, C.W. Hung1 and H.B. Chen2
1Department of Civil Engineering, National Chung Hsing University, Taichung, Taiwan
C.P. Tsai, C.W. Hung, H.B. Chen, "Simulation of the Shoreline Change behind a Submerged Permeable Breakwater", in , (Editors), "Proceedings of the Seventh International Conference on Engineering Computational Technology", Civil-Comp Press, Stirlingshire, UK, Paper 82, 2010. doi:10.4203/ccp.94.82
Keywords: submerged permeable breakwater, shoreline change, time-dependent mild-slope equation, continuity equation of sediment.
Summary
When waves pass a submerged permeable breakwater, the wave heights may decay over the breakwater as a result of wave energy dissipation and the induced circulation current system behind the structure is likely to make the sand deposit. On the other hand, the porous breakwater has the function of ecological restoration and has less impact on the coastal environment. Thus it is used increasingly by costal engineers for prevention of coastal erosion. Significant literature has paid attention to the wave transformation passing the submerged breakwater. In this paper, a numerical model is presented for simulating the shoreline change in the lee of a permeable submerged breakwater.
In the past, many numerical models were proposed to simulate the shoreline changes. These models include two-dimensional line models [1,2,3,4] for the long-term shoreline change or a three-dimensional model [5] for the short-term topography variation. However, previous models considered the coastal structure as an impermeable one, rather than the porous structure considered in this paper. In the present model, the wave field around the submerged permeable breakwater was first calculated based on the time-dependent mild slope equation proposed by Tsai et al. [6] that the porous parameters of the structure were involved. Then, the long-term shoreline change model is then established based on the continuity equation of the sediment, in which the longshore sediment transportation due to the effect of the wave diffraction is calculated using the breaking wave energy flux. The movable-bed experiments were also conducted in a two-dimensional wave basin for verifying the simulated results. The comparisons show that the numerical results of the wave height variations and the shoreline change are well in agreement with the experimental results. References
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