Phase shifting, dispersion variation and defocusing suppression in wave breaking

TL;DR

This study investigates the physical processes in deep water wave breaking, highlighting the limitations of existing models and proposing advanced numerical methods to better predict phase shifts and dispersion effects during wave breaking.

Contribution

The paper introduces a coupled FNP and Navier-Stokes model to analyze wave breaking, revealing the causes of phase shift inaccuracies in traditional eddy viscosity models.

Findings

EVBM accurately predicts energy dissipation and amplitude spectra.

EVBM fails to accurately capture phase shifting during breaking.

Wave dispersion relation shifts upward with breaking intensity, affecting wave propagation.

Abstract

We present an investigation of the fundamental physical processes involved in deep water wave breaking. Our motivation is to identify the underlying reason causing the deficiency of the eddy viscosity breaking model (EVBM) in predicting surface elevation for strongly nonlinear waves. Owing to the limitation of experimental methods in the provision of high-resolution flow information, we propose a numerical methodology by developing an EVBM enclosed standalone fully-nonlinear quasi-potential (FNP) flow model and a coupled FNP plus Navier-Stokes flow model. The numerical models were firstly verified with a wave train subject to modulational instability, then used to simulate a series of broad-banded focusing wave trains under non-, moderate- and strong-breaking conditions. A systematic analysis was carried out to investigate the discrepancies of numerical solutions produced by the two models in surface elevation and other important physical properties. It is found that EVBM predicts accurately the energy dissipated by breaking and the amplitude spectrum of free waves in terms of magnitude, but fails to capture accurately breaking induced phase shifting. The shift of phase grows with breaking intensity and is especially strong for high wavenumber components. This is identified as a cause of the upshift of wave dispersion relation, which increases the frequencies of large wavenumber components. Such a variation drives large-wavenumber components to propagate at nearly the same speed, which is significantly higher than the linear dispersion levels. This suppresses the instant dispersive spreading of harmonics after the focal point, prolonging the lifespan of focused waves and expanding their propagation space.