Abstract

For sufficiently directionally spread surface gravity wave groups, the set-down of the wave-averaged free surface, first described by Longuet-Higgins and Stewart (J. Fluid Mech. vol. 13, 1962, pp. 481–504), can turn into a set-up. Using a multiple-scale expansion for two crossing wave groups, we examine the structure and magnitude of this wave-averaged set-up, which is part of a crossing wave pattern that behaves as a modulated partial standing wave: in space, it consists of a rapidly varying standing-wave pattern slowly modulated by the product of the envelopes of the two groups; in time, it grows and decays on the slow time scale associated with the translation of the groups. Whether this crossing wave pattern actually enhances the surface elevation at the point of focus depends on the phases of the linear wave groups, unlike the set-down, which is always negative and inherits the spatial structure of the underlying envelope(s). We present detailed laboratory measurements of the wave-averaged free surface, examining both single wave groups, varying the degree of spreading from small to very large, and the interaction between two wave groups, varying both the degree of spreading and the crossing angle between the groups. In both cases, we find good agreement between the experiments, our simple expressions for the set-down and set-up, and existing second-order theory based on the component-by-component interaction of individual waves with different frequencies and directions. We predict and observe a set-up for wave groups with a Gaussian angular amplitude distribution with standard deviations of above $30{-}40^{\circ }$ ($21{-}28^{\circ }$ for energy spectra), which is relatively large for realistic sea states, and for crossing sea states with angles of separation of $50{-}70^{\circ }$ and above, which are known to occur in the ocean.

Highlights

  • In order to satisfy the nonlinear kinematic and dynamic free-surface boundary conditions, linear freely propagating surface gravity waves are accompanied by nonlinear bound components

  • Using a multiple-scale expansion for two crossing wave groups, we examine the structure and magnitude of this wave-averaged set-up, which is part of a crossing wave pattern that behaves as a modulated partial standing wave: in space, it consists of a rapidly varying standing-wave pattern slowly modulated by the product of the envelopes of the two groups; in time, it grows and decays on the slow time scale associated with the translation of the groups

  • We compare our experimental results with predictions for the wave-averaged free surface based on the parameters estimated from the linear signal in the two categories we consider: spreading tests and crossing tests

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Summary

Introduction

In order to satisfy the nonlinear kinematic and dynamic free-surface boundary conditions, linear freely propagating surface gravity waves are accompanied by nonlinear bound components. In the unidirectional case, the bound frequency-difference terms cause a depression in the wave-averaged surface elevation on the scale of the wave group, often referred to as a set-down (Longuet-Higgins & Stewart 1962). All of the experimental studies that we are aware of have been limited to small degrees of directional spreading and have not observed the formation of a set-up, with the exception of Toffoli et al (2011), who did conduct experiments with crossing wave systems at crossing angles up to 40◦, but did not examine the occurrence of a set-up.

Second-order theory
A single narrow-banded and narrowly spread wave group: set-down
Two crossing groups: set-up and set-down
Experimental method
FloWave and gauge layout
Crossing
Category A – spreading tests
Category B – crossing tests
Harmonic separation
Estimation of spectral parameters
Estimation of measured directional spectrum
Measurement error and repeatability
Results
Residual tank motion ηI Low-pass filtered ηI
The role of phase
Conclusions
Two-phase harmonic extraction
Four-phase harmonic extraction
Full Text
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