Abstract

AbstractDetailed measurements are presented of velocities and turbulence under a large‐scale regular plunging breaking wave in a wave flume. Measurements were obtained at 12 cross‐shore locations around a mobile medium‐sand breaker bar. They focused particularly on the dynamics of the wave bottom boundary layer (WBL) and near‐bed turbulent kinetic energy (TKE), measured with an Acoustic Concentration and Velocity Profiler (ACVP). The breaking process and outer flow hydrodynamics are in agreement with previous laboratory and field observations of plunging waves, including a strong undertow in the bar trough region. The WBL thickness matches with previous studies at locations offshore from the bar crest, but it increases near the breaking‐wave plunge point. This relates possibly to breaking‐induced TKE or to the diverging flow at the shoreward slope of the bar. Outer flow TKE is dominated by wave breaking and exhibits strong spatial variation with largest TKE above the breaker bar crest. Below the plunge point, breaking‐induced turbulence invades the WBL during both crest and trough half cycle. This results in an increase in the time‐averaged TKE in the WBL (with a factor 3) and an increase in peak onshore and offshore near‐bed Reynolds stresses (with a factor 2) from shoaling to breaking region. A fraction of locally produced TKE is advected offshore over a distance of a few meters to shoaling locations during the wave trough phase, and travels back onshore during the crest half cycle. The results imply that breaking‐induced turbulence, for large‐scale conditions, may significantly affect near‐bed sediment transport processes.

Highlights

  • Motivated by the need to improve understanding of cross-shore sediment transport processes in the nearshore region, a number of laboratory [e.g., Ting and Kirby, 1994, 1995; Yoon and Cox, 2010] and field [e.g., Ruessink, 2010; Feddersen, 2012] studies have addressed the effects of wave breaking on hydrodynamics

  • While wave breaking is highlighted as the dominant source of turbulent kinetic energy (TKE) production in the surf zone [Thornton and Guza, 1983; Ruessink, 2010; Yoon and Cox, 2010], bed-friction-generated turbulence can contribute importantly to turbulence in the lower water column [Feddersen, 2012; Brinkkemper et al, 2015]

  • In the case of a plunging breaker, turbulent vortices are formed at the wave front [Kimmoun and Branger, 2007; Sumer et al, 2013] and a major part of the breaking-induced TKE is dissipated within the turbulent bore above wave trough level [Svendsen, 1987; Govender et al, 2002]

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Summary

Introduction

Motivated by the need to improve understanding of cross-shore sediment transport processes in the nearshore region, a number of laboratory [e.g., Ting and Kirby, 1994, 1995; Yoon and Cox, 2010] and field [e.g., Ruessink, 2010; Feddersen, 2012] studies have addressed the effects of wave breaking on hydrodynamics. TKE profiles have been found to vary in the cross-shore direction and depend on the bed topography, with highest TKE found at the breaker bar crest and lower TKE above the bar trough [Scott et al, 2005; Yoon and Cox, 2010]

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