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首页> 外文期刊>Journal of physical oceanography >An Analytical Spectral Model for Infragravity Waves over Topography in Intermediate and Shallow Water under Nonbreaking Conditions
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An Analytical Spectral Model for Infragravity Waves over Topography in Intermediate and Shallow Water under Nonbreaking Conditions

机译：An Analytical Spectral Model for Infragravity Waves over Topography in Intermediate and Shallow Water under Nonbreaking Conditions

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摘要

The theoretical model for group-forced infragravity (IG) waves in shallow water is not well established for nonbreaking conditions. In the present study, analytical solutions of the group-forced IG waves at O(beta(1)) (beta(1) = h(x)/(Delta kh), h(x) = bottom slope, Delta k 5 group wavenumber, h 5 depth) in intermediate water and at O(beta(-1)(1)) in shallow water are derived separately. In case of off-resonance [beta(1)mu(-1) = O(beta(1)), where mu = 1 -c(g)(2)/(gh) is the resonant departure parameter, c(g) = group speed] in intermediate water, additional IG waves in quadrature with the wave group forcing (hereinafter, the nonequilibrium response or component) are induced at O(beta(1)) relative to the equilibrium bound IG wave solution of LonguetHiggins and Stewart (1962) in phase with the wave group. The present theory indicates that the nonequilibrium response is mainly attributed to the spatial variation of the equilibrium bound IG wave amplitude instead of group-forcing. In case of near-resonance [beta(1)mu(-1) = O(1)] in shallow water; however, both the equilibrium and nonequilibrium components are similar to O(beta(-1)(1)) at the leading order. Based on the nearly-resonant solution, the shallow water limit of the local shoaling rate of bound IG waves over a plane sloping beach is derived to be similar to h(-1) for the first time. The theoretical predictions compare favorably with the laboratory experiment by Van Noorloos (2003) and the present numerical model results generated using SWASH. Based on the proposed solution, the group-forced IGwaves over a symmetric shoal are investigated. In case of offresonance, the solution predicts a roughly symmetric reversible spatial evolution of the IG wave amplitude, while in cases of near to full resonance the IG wave is significantly amplified over the shoal with asymmetric irreversible spatial evolution.

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