Hostname: page-component-78c5997874-ndw9j Total loading time: 0 Render date: 2024-11-17T14:53:53.975Z Has data issue: false hasContentIssue false

Direct numerical simulations of bifurcations in an air-filled rotating baroclinic annulus

Published online by Cambridge University Press:  09 August 2006

ANTHONY RANDRIAMAMPIANINA
Affiliation:
Institut de Recherche sur les Phénomènes Hors Equilibrie, UMR 6594 CNRS, Technopôle de Château-Gombert, 49, rue Frédéric Jolie-Curie, BP 146, 13384 Marseille cedex 13, France
WOLF-GERRIT FRÜH
Affiliation:
School of Engineering and Physical Sciences, Heriot-Watt University, Riccarton, Edinburgh EH14 4AS, UK
PETER L. READ
Affiliation:
Atmospheric, Oceanic & Planetary Physics, University of Oxford, Clarendon Laboratory, Oxford OX1 3PU, UK
PIERRE MAUBERT
Affiliation:
Institut de Recherche sur les Phénomènes Hors Equilibrie, UMR 6594 CNRS, Technopôle de Château-Gombert, 49, rue Frédéric Jolie-Curie, BP 146, 13384 Marseille cedex 13, France

Abstract

Three-dimensional direct numerical simulations (DNS) of the nonlinear dynamics and a route to chaos in a rotating fluid subjected to lateral heating are presented here and discussed in the context of laboratory experiments in the baroclinic annulus. Following two previous preliminary studies, the fluid used is air rather than a liquid as used in all other previous work. This study investigates a bifurcation sequence from the axisymmetric flow to a number of complex flows.

The transition sequence, on increase of the rotation rate, from the axisymmetric solution via a steady fully developed baroclinic wave to chaotic flow, followed a variant of the classical quasi-periodic bifurcation route, starting with a subcritical Hopf and associated saddle-node bifurcation. This was followed by a sequence of two supercritical Hopf-type bifurcations, first to an amplitude vacillation, then to a three-frequency quasi-periodic modulated amplitude vacillation (MAV), and finally to a chaotic (MAV). In the context of the baroclinic annulus this sequence is unusual as the vacillation is usually found on decrease of the rotation rate from the steady wave flow.

Further transitions of a steady wave with a higher wavenumber pointed to the possibility that a barotropic instability of the sidewall boundary layers and the subsequent breakdown of these barotropic vortices may play a role in the transition to structural vacillation and, ultimately, geostrophic turbulence.

Type
Papers
Copyright
© 2006 Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)