Hostname: page-component-84b7d79bbc-7nlkj Total loading time: 0 Render date: 2024-07-29T21:18:21.686Z Has data issue: false hasContentIssue false

Modelling the morning glory of the Gulf of Carpentaria

Published online by Cambridge University Press:  25 March 2002

ANNE PORTER
Affiliation:
Department of Mathematics and Statistics, The King's Buildings, University of Edinburgh, Edinburgh EH9 3JZ, Scotland, UK; e-mail: noel@maths.ed.ac.uk Present address: Department of Mathematics, University of Bristol, University Walk, Bristol BS8 1TW, UK.
NOEL F. SMYTH
Affiliation:
Department of Mathematics and Statistics, The King's Buildings, University of Edinburgh, Edinburgh EH9 3JZ, Scotland, UK; e-mail: noel@maths.ed.ac.uk

Abstract

The morning glory is a meteorological phenomenon which occurs in northern Australia and takes the form of a series of roll clouds. The morning glory is generated by the interaction of nocturnal seabreezes over Cape York Peninsula and propagates in a south-westerly direction over the Gulf of Carpentaria. In the present work, it is shown that the morning glory can be modelled by the resonant flow of a two-layer fluid over topography, the topography being the mountains of Cape York Peninsula. In the limit of a deep upper layer, the equations of motion reduce to a forced Benjamin–Ono equation. In this context, resonant means that the underlying flow velocity of the seabreezes is near a linear long-wave velocity for one of the long-wave modes. The morning glory is then modelled by the undular bore (simple wave) solution of the modulation equations for the Benjamin–Ono equation. This modulation solution is compared with full numerical solutions of the forced Benjamin–Ono equation and good agreement is found when the wave amplitudes are not too large. The reason for the difference between the numerical and modulation solutions for large wave amplitude is also discussed. Finally, the predictions of the modulation solution are compared with observational data on the morning glory and good agreement is found for the pressure jump due to the lead wave of the morning glory, but not for the speed and half-width of this lead wave. The reasons for this are discussed.

Type
Research Article
Copyright
© 2002 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.)