eISSN 1942-2466
Vol. 2, 2010
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J. Adv. Model. Earth Syst., Vol. 2, Art.#14, 20 pp.

Published Online 22 Dec. '10

Slow manifolds and multiple equilibria in stratocumulus-capped boundary layers

Christopher Bretherton, Junya Uchida, Peter N. Blossey

Abstract


In marine stratocumulus-capped boundary layers under strong inversions, the timescale for thermodynamic adjustment is roughly a day, much shorter than the multiday timescale for inversion height adjustment. Slow-manifold analysis is introduced to exploit this timescale separation when boundary layer air columns experience only slow changes in their boundary conditions. Its essence is that the thermodynamic structure of the boundary layer remains approximately slaved to its inversion height and the instantaneous boundary conditions; this slaved structure determines the entrainment rate and hence the slow evolution of the inversion height.

Slow-manifold analysis is shown to apply to mixed-layer model and large-eddy simulations of an idealized nocturnal stratocumulus- capped boundary layer; simulations with different initial inversion heights collapse onto single relationships of cloud properties with inversion height. Depending on the initial inversion height, the simulations evolve toward a shallow thin-cloud boundary layer or a deep, well-mixed thick cloud boundary layer. In the large-eddy simulations, these evolutions occur on two separate slow manifolds (one of which becomes unstable if cloud droplet concentration is reduced). Applications to analysis of stratocumulus observations and to pockets of open cells and ship tracks are proposed.


 Article Spotlight
Figure 18: Schematic cross-section through a pocket of open cells (POC), with precipitating cumuli detraining into thin broken stratocumulus surrounded by thicker overcast stratocumulus. Inversion height zinv is dashed. Streamlines descend from the mid-troposphere into the inversion, diverging from the POC into the overcast region, where air is entrained into the boundary layer. Wide arrow length indicates subsidence rate; eddy-like symbols indicate entrainment. Horizontal-mean divergence is assumed to be zero above the boundary layer for graphical simplicity.
Cite this article in JAMES:
Bretherton, C., J. Uchida and P. N. Blossey, (2010): Slow manifolds and multiple equilibria in stratocumulus-capped boundary layers. J. Adv. Model. Earth Syst., 2, Art.#14, 20 pp., doi:10.3894/JAMES.2010.2.14
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