Atmosphere–Ocean Coupled Energy Budgets of Tropical Convective Discharge–Recharge Cycles

Author:

Wolding Brandon1ORCID,Rydbeck Adam2,Dias Juliana3,Ahmed Fiaz4,Gehne Maria1,Kiladis George3,Dellaripa Emily M. Riley5,Chen Xingchao6,McCoy Isabel L.17

Affiliation:

1. a Cooperative Institute for Research in Environmental Sciences, University of Colorado Boulder, Boulder, Colorado

2. b U.S. Naval Research Laboratory, Stennis Space Center, Mississippi

3. c National Oceanic and Atmospheric Administration/Physical Sciences Laboratory, Boulder, Colorado

4. d Department of Atmospheric and Oceanic Sciences, University of California, Los Angeles, Los Angeles, California

5. e Department of Atmospheric Science, Colorado State University, Fort Collins, Colorado

6. f Department of Meteorology and Atmospheric Science, Center for Advanced Data Assimilation and Predictability Techniques, The Pennsylvania State University, University Park, Pennsylvania

7. g National Oceanic and Atmospheric Administration/Chemical Sciences Laboratory, Boulder, Colorado

Abstract

Abstract An energy budget combining atmospheric moist static energy (MSE) and upper ocean heat content (OHC) is used to examine the processes impacting day-to-day convective variability in the tropical Indian and western Pacific Oceans. Feedbacks arising from atmospheric and oceanic transport processes, surface fluxes, and radiation drive the cyclical amplification and decay of convection around suppressed and enhanced convective equilibrium states, referred to as shallow and deep convective discharge–recharge (D–R) cycles, respectively. The shallow convective D–R cycle is characterized by alternating enhancements of shallow cumulus and stratocumulus, often in the presence of extensive cirrus clouds. The deep convective D–R cycle is characterized by sequential increases in shallow cumulus, congestus, narrow deep precipitation, wide deep precipitation, a mix of detached anvil and altostratus and altocumulus, and once again shallow cumulus cloud types. Transitions from the shallow to deep D–R cycle are favored by a positive “column process” feedback, while discharge of convective instability and OHC by mesoscale convective systems (MCSs) contributes to transitions from the deep to shallow D–R cycle. Variability in the processes impacting MSE is comparable in magnitude to, but considerably more balanced than, variability in the processes impacting OHC. Variations in the quantity of atmosphere–ocean coupled static energy (MSE + OHC) result primarily from atmospheric and oceanic transport processes, but are mainly realized as changes in OHC. MCSs are unique in their ability to rapidly discharge both lower-tropospheric convective instability and OHC.

Funder

Department of Water Resources

Earth System Research Laboratories

Office of Naval Research Global

NASA CYGNSS

DOE Global Model Analysis

National Science Foundation

Publisher

American Meteorological Society

Subject

Atmospheric Science

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