Three-dimensional wave breaking

Journal Article (2024)
Author(s)

M.L. McAllister (University of Oxford)

S. Draycott (The University of Manchester)

R. Calvert (The University of Edinburgh)

T. Davey (The University of Edinburgh)

F. Dias (University College Dublin, ENS Paris-Saclay)

T.S. van den Bremer (TU Delft - Environmental Fluid Mechanics)

Research Group
Environmental Fluid Mechanics
DOI related publication
https://doi.org/10.1038/s41586-024-07886-z Final published version
More Info
expand_more
Publication Year
2024
Language
English
Research Group
Environmental Fluid Mechanics
Issue number
8030
Volume number
633
Article number
8798
Pages (from-to)
601–607
Downloads counter
249
Reuse Rights

Other than for strictly personal use, it is not permitted to download, forward or distribute the text or part of it, without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license such as Creative Commons.

Abstract

Although a ubiquitous natural phenomenon, the onset and subsequent process of surface wave breaking are not fully understood. Breaking affects how steep waves become and drives air–sea exchanges1. Most seminal and state-of-the-art research on breaking is underpinned by the assumption of two-dimensionality, although ocean waves are three dimensional. We present experimental results that assess how three-dimensionality affects breaking, without putting limits on the direction of travel of the waves. We show that the breaking-onset steepness of the most directionally spread case is double that of its unidirectional counterpart. We identify three breaking regimes. As directional spreading increases, horizontally overturning ‘travelling-wave breaking’ (I), which forms the basis of two-dimensional breaking, is replaced by vertically jetting ‘standing-wave breaking’ (II). In between, ‘travelling-standing-wave breaking’ (III) is characterized by the formation of vertical jets along a fast-moving crest. The mechanisms in each regime determine how breaking limits steepness and affects subsequent air–sea exchanges. Unlike in two dimensions, three-dimensional wave-breaking onset does not limit how steep waves may become, and we produce directionally spread waves 80% steeper than at breaking onset and four times steeper than equivalent two-dimensional waves at their breaking onset. Our observations challenge the validity of state-of-the-art methods used to calculate energy dissipation and to design offshore structures in highly directionally spread seas.