Abstract

The dispersive characteristics of unidirectional irregular waves propagating and breaking over a mildly sloping beach are examined using a highly-resolved laboratory dataset. Cross-spectral analyses are used to determine the cross-shore evolution of (single-valued) dominant wavenumber κ and phase velocity c spectra, and lead to the identification of four different regimes of propagation: I - a linear regime where short waves mostly propagate as free components; II - a shoaling regime where non-linear effects at high harmonics are significant but primary components follow the linear wave dispersion relation; III - a shoaling regime near the mean breaking point location, where amplitude dispersion effects at primary components are important; IV - a surf zone regime, where all components propagate slightly faster than non-dispersive shallow water waves. Bispectral analyses performed onshore of the shoaling region show that the presence of forced energy at high harmonics, which originate from non-linear interactions between triads of frequencies, are responsible for the deviations of wavenumber and phase velocity spectral estimates from predictions by the linear dispersion relation, confirming the findings from previous field-based studies. A Boussinesq approximation of the non-linear energy exchanges between triads is then used to quantify the relative amount of forced energy at high harmonics and explain the differences in dispersion properties observed in the shoaling region between broad and narrow-band spectra. Larger relative amounts of forced energy at high frequencies, which suggest more efficient non-linear energy transfers, are found to be associated with larger deviations of dominant κ and c from predictions by the linear dispersion relation.

Highlights

  • Wind-generated surface gravity waves are the principal driver of nearshore dynamics

  • Stage II (Ur ∼ 0.3) is interesting as it simultaneously shows significant non-linear effects at high harmonics, which are evidenced by the large deviations of κ and c spectra from predictions by the linear wave dispersion relation, and a clearly linear spatial field for the primary components

  • Less energy was imposed during A3 as compared to A2, the narrow-banded conditions promoted relatively more important non-linear energy transfers towards high harmonics such that phase velocity at 2fp and 3fp were found equal to those at the peak frequency

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Summary

Introduction

Wind-generated surface gravity waves (hereafter short waves) are the principal driver of nearshore dynamics. As opposed to non-linear resonant interactions between quadruplets in deep water (Hasselmann, 1962), which require very large distances to be effective, non-linear coupling between triads in nearshore areas are non- or near-resonant and can be very efficient in transforming incident wave spectra over just few typical wavelengths (e.g., see Freilich et al, 1984, and the references therein) As both forced (or ’bound’) and free components of directionally spread seas can co-exist in a wave field, there is no longer a unique relation between a frequency and wavenumber (e.g. Herbers and Guza, 1994).

Experimental dataset
Computation of wavenumber and phase velocity spectra
Computation of bispectra
Non-linear energy transfers
Wavenumber and phase velocity spectra of shoaling and surf zone waves
Role of non-linear energy transfers on κ and c
Findings
Discussion and concluding remarks
Full Text
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