Highly directionally spread, overturning breaking waves modelled with Smoothed Particle Hydrodynamics

A case study involving the Draupner wave

Journal Article (2021)
Authors

Taiga Kanehira (Hiroshima University)

Mark L. McAllister (University of Oxford)

Samuel Draycott (The University of Manchester)

T. Nakashima (Hiroshima University)

Naokazu Taniguchi (Hiroshima University)

David Ingram (The University of Edinburgh)

Ton S. Van Den Bremer (University of Oxford, Environmental Fluid Mechanics)

Hidemi Mutsuda (Hiroshima University)

Affiliation
Environmental Fluid Mechanics
Copyright
© 2021 T. Kanehira, M. L. McAllister, S. Draycott, T. Nakashima, N. Taniguchi, D. M. Ingram, T.S. van den Bremer, H. Mutsuda
To reference this document use:
https://doi.org/10.1016/j.ocemod.2021.101822
More Info
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Publication Year
2021
Language
English
Copyright
© 2021 T. Kanehira, M. L. McAllister, S. Draycott, T. Nakashima, N. Taniguchi, D. M. Ingram, T.S. van den Bremer, H. Mutsuda
Affiliation
Environmental Fluid Mechanics
Volume number
164
DOI:
https://doi.org/10.1016/j.ocemod.2021.101822
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Abstract

Wave breaking in the ocean affects the height of extreme waves, energy dissipation, and interaction between the atmosphere and upper ocean. Numerical modelling is a critical step in understanding the physics of wave breaking and offers insight that is hard to gain from field data or experiments. High-fidelity numerical modelling of three-dimensional breaking waves is extremely challenging. Conventional grid-based numerical methods struggle to model the steep and double-valued free surfaces that occur during wave breaking. The Smoothed Particle Hydrodynamics (SPH) method does not fall prey to these issues. Herein, we examine the SPH method's ability to model highly directionally spread overturning breaking waves by numerically reproducing the experiments presented in McAllister et al. (2019). We find that the SPH method reproduces the experimental observations well; when comparing experimental and numerical measurements we achieve coefficient of determination values of 0.92−0.95, with some smaller-scale features less well reproduced owing to finite resolution. We also examine aspects of the simulated wave's geometry and kinematics and find that existing breaking criteria are difficult to apply in highly directionally spread conditions.

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