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Testing and calibrating parametric wave transformation models on natural beaches

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TLDR
In this article, the authors compare different parametric wave transformation models with extensive observations from six field experiments on barred and unbarred beaches and show that the default model provides the best predictions for all data records or at all experiments.
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This article is published in Coastal Engineering.The article was published on 2008-03-01 and is currently open access. It has received 92 citations till now. The article focuses on the topics: Wave height.

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Wave-Driven Circulation of a Coastal Reef–Lagoon System

TL;DR: The response of the circulation of a coral reef system in Kaneohe Bay, Hawaii, to incident wave forcing was investigated using field data collected during a 10-month experiment as mentioned in this paper.
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A note on wave energy dissipation over steep beaches

TL;DR: This article revisited the derivation of the parametric surf zone model proposed by Baldock et al. and showed that a consistent use of the proposed Rayleigh distribution for surf zone wave heights results in modification of the expressions for the bulk dissipation rate and enhanced dissipation levels on steep beaches and over-saturated surf zone conditions.
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Quantifying wave attenuation to inform coastal habitat conservation

TL;DR: In this article, the authors re-analyzed existing wave attenuation studies in kelp, mangrove, marsh and seagrass habitats and found that much of the variation in wave attenuations can be explained by differences in vegetation characteristics and by the change in bulk drag with flow conditions.
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Evaluation of wave runup predictions from numerical and parametric models

TL;DR: In this article, a numerical model is used to simulate the storm-driven runup to compare to the parameterized model and then develop an approach to improve the accuracy of the parameterization.
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Modeling of depth-induced wave breaking under finite depth wave growth conditions

TL;DR: In this paper, a rescaling of the Battjes and Janssen (1978) bore-based model for depth-induced breaking, considering both sloping bed surf zone situations and finite depth wave growth conditions, was proposed.
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Journal ArticleDOI

Radiation stresses in water waves; a physical discussion, with applications

TL;DR: The radiation stresses in water waves play an important role in a variety of oceanographic phenomena, for example in the change in mean sea level due to storm waves (wave set-up), the generation of "surf-beats", the interaction of waves with steady currents, and the steepening of short gravity waves on the crests of longer waves as discussed by the authors.
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Energy loss and set-up due to breaking of random waves

TL;DR: In this article, a model was developed for the prediction of the dissipation of energy in random waves breaking on a beach and the probability of occurrence of breaking waves was estimated on the basis of a wave height distribution with an upper cut-off which in shallow water is determined mainly by the local depth.
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Alternative form of Boussinesq equations for nearshore wave propagation

TL;DR: In this paper, a new form of the Boussinesq equations is derived using the velocity at an arbitrary distance from the still water level as the velocity variable instead of the commonly used depth-averaged velocity.
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Radiation stress and mass transport in gravity waves, with application to `surf-beats'

TL;DR: In this article, the second-order currents and changes in mean surface level which are caused by gravity waves of non-uniform amplitude are investigated, and the effects are interpreted in terms of the radiation stresses in the waves.
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Transformation of wave height distribution

TL;DR: In this paper, the authors reviewed earlier models of random wave transformation and described the transformation of waves, including dissipation due to breaking and bottom friction, by an energy flux balance model, and compared results from random wave experiments in the laboratory and from an extensive set of field measurements.
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Frequently Asked Questions (15)
Q1. What are the contributions in this paper?

In this paper, several parametric models for the transformation of wave heights across the surfzone were tested and calibrated with observations collected along crossshore transects at 6 experiments on barred and unbarred beaches. 

Model accuracy decreases with decreasing water depth, partially owing to the accumulation of errors with increasing distance from the location of model initialization. 

To tune the models accurately, data must span the surfzone, which may require at least three to five sensors depending on tidal and wave height ranges. 

To optimize predictions of the cross-shore distribution of wave heights, data are needed from at least two sensors spanning the surfzone, which changes in width and location with changing wave conditions and tidal levels. 

The bathymetry was surveyed approximately every other day from about 8-m water depth to above the high tide shoreline along cross-shore transects located about 20 m alongshore of the instrumented transects. 

The energyweighted (centroidal) frequency was used as the representative frequency when wave spectra were available (Duck94, SandyDuck, SwashX, and NCEX). 

Root-mean-square wave heights at the most offshore sensors ranged from 0.19 to 3.93 m (Egmond) and from 0.12 to 1.84 m (Terschelling). 

At SandyDuck, three sensors are needed close to the shore to ensure that at least two sensors are located in the surfzone during all tidal stages for small waves, and at least one (or ideally two) sensors are needed in deeper water to span the width of the wider surfzone during large waves (not shown). 

Root-mean-square wave heights at the most offshore sensor (h ≈ 5 m) ranged from 0.20 to 2.10 m (SandyDuck) and from 0.14 to 2.92 m (Duck94). 

The dependence of the best-fit γ on the offshore wave height may be related to variations in B (which relates the dissipation in a hydraulic jump to that in a breaking wave) or to other parameterized processes, such as infragravity wave generation and differences in breaking-wave dissipation in spilling and plunging waves. 

The larger spread at Egmond and Terschelling (Figure 8, cyan and yellow curves) likely occurs because the lack of sensors in shallow water decreases best-fit γ for small Ho. 

Similar to previous results [Ruessink, personal communication], use of γ = 0.42 in the TG model for large deep-water waves (Ho > 1.5 m) causes too much dissipation in the outer surfzone, and thus the predicted waves are smaller than the observed waves. 

use of the default value of γ = 0.42 in the TG model may result in significant underprediction of surfzone wave heights when Ho is large. 

1"Q "lnQ = H rmsH m# $ %& ' (2, (4)where Hm is found by extending the Miche criterion for the maximum height of periodic waves of constant form [Miche, 1951] to! 

Inclusion of the data from Egmond and Terschelling reduces the values of γ estimated for small Ho (see above), but does not change significantly the values estimated for Ho > 1.5 m.