4.6 Article

Convective organization and eastward propagating equatorial disturbances in a simple excitable system

Journal

QUARTERLY JOURNAL OF THE ROYAL METEOROLOGICAL SOCIETY
Volume 146, Issue 730, Pages 2297-2314

Publisher

WILEY
DOI: 10.1002/qj.3792

Keywords

convection; equatorial dynamics; geophysical fluid dynamics; Madden-Julian Oscillation; physical phenomenon

Funding

  1. Leverhulme Trust [RPG-2015-186]
  2. NERC (the ParaCon Project)
  3. Newton Fund (CSSP China)
  4. NERC [NE/T00942X/1] Funding Source: UKRI

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We describe and illustrate a mechanism whereby convective aggregation and eastward propagating equatorial disturbances, which are similar in some respects to the Madden-Julian Oscillation (MJO), arise. We construct a simple explicit system consisting only of the shallow-water equations plus a humidity variable; moisture enters via evaporation from a wet surface, is transported by the flow and removed by condensation, thus producing an anomaly in the height field. For a broad range of parameters the system is excitable even when linearly stable, with condensation producing convergence and gravity waves that, acting together, trigger more condensation. On the equatorial beta-plane the convection first aggregates near the Equator, generating patterns related to those encountered in the Matsuno-Gill problem. However, the pattern is unstable and more convection is triggered on its eastern edge, leading to a self-sustaining precipitating disturbance that progresses eastward. The propagation is eastward because the warm, moist converging air from the east induced by the Matsuno-Gill pattern is more convectively unstable than the converging air from the west. The pattern is confined to a region within a few deformation radii of the Equator, as here the convection can create the convergence needed to organize itself into a self-sustaining pattern; thus, smaller values of the beta parameter give rise to a wider disturbance. Formation of the disturbance preferentially occurs where the surface is warmer, and sufficient time (typically a few tens of days) must pass before conditions arise that enable the disturbance to reform, a well-known characteristic of the MJO. The speed of the disturbance depends on the efficiency of evaporation and the heat released by condensation, and is typically a few metres per second, much less than the Kelvin wave speed.

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