Abstract

Abstract. The study of the adjustment to equilibrium by a stratified fluid in a rotating reference frame is a classical problem in geophysical fluid dynamics. We consider the fully nonlinear, stratified adjustment problem from a numerical point of view. We present results of smoothed dam break simulations based on experiments in the published literature, with a focus on both the wave trains that propagate away from the nascent geostrophic state and the geostrophic state itself. We demonstrate that for Rossby numbers in excess of roughly 2 the wave train cannot be interpreted in terms of linear theory. This wave train consists of a leading solitary-like packet and a trailing tail of dispersive waves. However, it is found that the leading wave packet never completely separates from the trailing tail. Somewhat surprisingly, the inertial oscillations associated with the geostrophic state exhibit evidence of nonlinearity even when the Rossby number falls below 1. We vary the width of the initial disturbance and the rotation rate so as to keep the Rossby number fixed, and find that while the qualitative response remains consistent, the Froude number varies, and these variations are manifested in the form of the emanating wave train. For wider initial disturbances we find clear evidence of a wave train that initially propagates toward the near wall, reflects, and propagates away from the geostrophic state behind the leading wave train. We compare kinetic energy inside and outside of the geostrophic state, finding that for long times a Rossby number of around one-quarter yields an equal split between the two, with lower (higher) Rossby numbers yielding more energy in the geostrophic state (wave train). Finally we compare the energetics of the geostrophic state as the Rossby number varies, finding long-lived inertial oscillations in the majority of the cases and a general agreement with the past literature that employed either hydrostatic, shallow-water equation-based theory or stratified Navier–Stokes equations with a linear stratification.

Highlights

  • Geostrophic balance, namely the balance between the pressure gradient and the Coriolis pseudoforce, is observed to hold to a good approximation for many large-scale motions in the atmosphere and the ocean

  • We subsequently identify the manner in which nonlinearity is exhibited in the problem, focusing on both the wave train and the geostrophic state and its inertial oscillations

  • Building on results based on shallow-water theory presented in Kuo and Polvani (1997), we have shown that by using the fully nonlinear incompressible Navier–Stokes equations, under the Boussinesq approximation, the waves that are ejected from the geostrophic state do not steepen to a shock

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Summary

Introduction

Geostrophic balance, namely the balance between the pressure gradient and the Coriolis pseudoforce, is observed to hold to a good approximation for many large-scale motions in the atmosphere and the ocean. There has been a great deal of published work on the linear problem (Ou, 1984; Gill, 1976; Middleton, 1987; Washington, 1964; Mihaljan, 1963), but little on the fully nonlinear one. This is partly because nonlinear problems rarely yield analytical solutions in closed form, and partly because numerical methods applied to the problem must accurately resolve multiple length scales

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