What determines meridional heat transport in climate models?

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Abstract

The annual mean maximum meridional heat transport (MHT MAX) differs by approximately 20% among coupled climate models. The value of MHT MAX can be expressed as the difference between the equator-topole contrast in absorbed solar radiation (ASR*) and outgoing longwave radiation (OLR*). As an example, in the Northern Hemisphere observations, the extratropics (defined as the region with a net radiative deficit) receive an 8.2-PW deficit of net solar radiation (ASR*) relative to the global average that is balanced by a 2.4-PW deficit of outgoing longwave radiation (OLR*) and 5.8 PW of energy import via the atmospheric and oceanic circulation (MHT MAX). The intermodel spread of MHT MAX in the Coupled Model Intercomparison Project Phase 3 (CMIP3) simulations of the preindustrial climate is primarily (R 2 5 0.72) due to differences in ASR* while model differences in OLR* are uncorrelated with theMHT MAX spread. The net solar radiation (ASR*) is partitioned into contributions from (i) the equator-to-pole contrast in incident radiation acting on the global average albedo and (ii) the equator-to-pole contrast of planetary albedo, which is further subdivided into components due to atmospheric and surface reflection. In the observations, 62% of ASR* is due to the meridional distribution of incident radiation, 33% is due to atmospheric reflection, and 5% is due to surface reflection. The intermodel spread in ASR* is due to model differences in the equator-to-pole gradient in planetary albedo, which are primarily a consequence of atmospheric reflection differences (92% of the spread), and is uncorrelated with differences in surface reflection. As a consequence, the spread in MHT MAX in climate models is primarily due to the spread in cloud reflection properties. © 2012 American Meteorological Society.

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Donohoe, A., & Battisti, D. S. (2012). What determines meridional heat transport in climate models? Journal of Climate, 25(11), 3832–3850. https://doi.org/10.1175/JCLI-D-11-00257.1

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