Abstract
This paper explores an idealized model of the ocean surface in which widely separated surface-wave packets and point vortices interact in two horizontal dimensions. We start with a Lagrangian which, in its general form, depends on the fields of wave action, wave phase, stream function and two additional fields that label and track the vertical component of vorticity. By assuming that the wave action and vorticity are confined to infinitesimally small, widely separated regions of the flow, we obtain model equations that are analogous to, but significantly more general than, the familiar system consisting solely of point vortices. We analyse stable and unstable harmonic solutions, solutions in which wave packets eventually coincide with point vortices (violating our assumptions), and solutions in which the wave vector eventually blows up. Additionally, we show that a wave packet induces a net drift on a passive vortex in the direction of wave propagation which is equivalent to Darwin drift. Generalizing our analysis to many wave packets and vortices, we examine the influence of wave packets on an otherwise unstable vortex street and show analytically, according to linear stability analysis, that the wave-packet-induced drift can stabilize the vortex street. The system is then numerically integrated for long times and an example is shown in which the configuration remains stable, which may be particularly relevant for the upper ocean.
Highlights
This paper explores an idealized model of the ocean surface in which widely separated surface-wave packets and point vortices interact in two horizontal dimensions
The dynamics is governed by wave action conservation (Longuet-Higgins & Stewart 1962; Whitham 1965), while the evolution of the phase obeys the equations of geometrical optics
Wave breaking in deep water occurs for waves with finite crest length, which implies that at the free surface the breaking-induced flow is characterized by a dipole structure (Peregrine 1999; Pizzo & Melville 2013)
Summary
This paper explores an idealized model of the ocean surface in which widely separated surface-wave packets and point vortices interact in two horizontal dimensions. Salmon converts wave action into vorticity, and vorticity is destroyed by viscosity In this initial study we consider only the ideal case, in which Ap and Γi are conserved. Wave packets advect the point vortices by their Bretherton flow. In the limit that the circulation of the vortices is much weaker than the wave action, the equations are equivalent to those diagnosing the motion of a particle in the presence of a uniformly translating cylinder. Numerical analysis demonstrates that vortex streets can be stable for long times in the presence of a wave packet.
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