NATURE GEOSCIENCE | VOL 5 | OCTOBER 2012 | www.nature.com/naturegeoscience 691
E
arth’s climate is determined by the flows of energy into and out
of the planet and to and from Earth’s surface. Geographical dis-
tributions of these energy flows at the surface are particularly
important as they drive ocean circulations, fuel the evaporation
of water from Earth’s surface and govern the planetary hydrologi-
cal cycle. Changes to the surface energy balance also ultimately
control how this hydrological cycle responds to the small energy
imbalances that force climate change
1
.
e seminal importance of Earth’s energy balance to climate has
been understood for more than a century. Although the earliest
depictions of the global annual mean energy budget of Earth date
to the beginning of the twentieth century
2,3
, the most significant
advance to our understanding of this energy balance occurred aſter
the space age in the 1960s. Among the highlights obtained from
early satellite views of Earth was the measurement of Earth’s albedo
(the ratio of outgoing flux of solar energy to incoming flux from
the Sun) at approximately 30% (ref. 4), thus settling a long-standing
debate on its magnitude — values ranged between 89% and 29%
(ref. 5) before these measurements. e sign and magnitude of the
net effect of clouds on the top-of-atmosphere (TOA) fluxes
6
was also
later established with the space-borne observations of the scanning
instrument on the Earth Radiation Budget Experiment (ERBE)
7
,
which better delineated between clear and cloudy skies. ERBE, and
later the Clouds and the Earth’s Radiant Energy System (CERES)
8
and the French Scanner for Radiation Budget
9
, confirmed that the
global cloud albedo effect was significantly larger than the green-
house effect of clouds. Although this was a major advance at the
time, determining the influence of clouds on atmospheric and sur-
face fluxes had to wait until the recent satellite measurements of the
vertical structure of clouds became available from the A-train
10
.
An update on Earth’s energy balance in light of the
latest global observations
Graeme L. Stephens
1
*, Juilin Li
1
, Martin Wild
2
, Carol Anne Clayson
3
, Norman Loeb
4
, Seiji Kato
4
,
Tristan L’Ecuyer
5
, Paul W. Stackhouse Jr
4
, Matthew Lebsock
1
and Timothy Andrews
6
Climate change is governed by changes to the global energy balance. At the top of the atmosphere, this balance is monitored
globally by satellite sensors that provide measurements of energy flowing to and from Earth. By contrast, observations at
the surface are limited mostly to land areas. As a result, the global balance of energy fluxes within the atmosphere or at
Earth’s surface cannot be derived directly from measured fluxes, and is therefore uncertain. This lack of precise knowledge of
surface energy fluxes profoundly affects our ability to understand how Earth’s climate responds to increasing concentrations
of greenhouse gases. In light of compilations of up-to-date surface and satellite data, the surface energy balance needs to be
revised. Specifically, the longwave radiation received at the surface is estimated to be significantly larger, by between 10 and
17 Wm
–2
, than earlier model-based estimates. Moreover, the latest satellite observations of global precipitation indicate that
more precipitation is generated than previously thought. This additional precipitation is sustained by more energy leaving
the surface by evaporation — that is, in the form of latent heat flux — and thereby offsets much of the increase in longwave
flux to the surface.
The global annual mean energy balance
e current revised depiction of the global annual mean energy
balance for the decade 2000–2010 is provided in Fig. B1. Although
the fluxes given are meant to be an average for that decade, the net
flux at the TOA (the difference of incoming minus outgoing fluxes)
varies on a variety of timescales
11,12
that include relatively large but
episodic changes by volcanic eruptions and a much smaller, more
systematic increase associated with increases in ocean heat storage
as Earth warms. For the decade considered, the average imbalance
is 0.6 = 340.2 − 239.7 − 99.9 Wm
–2
when these TOA fluxes are con-
strained to the best estimate ocean heat content (OHC) observations
since 2005 (refs 13,14). is small imbalance is over two orders of
magnitude smaller than the individual components that define it and
smaller than the error of each individual flux. e combined uncer-
tainty on the net TOA flux determined from CERES is ±4 Wm
–2
(95% confidence) due largely to instrument calibration errors
12,15
.
us the sum of current satellite-derived fluxes cannot determine
the net TOA radiation imbalance with the accuracy needed to track
such small imbalances associated with forced climate change
11
.
Despite this limitation, changes in the CERES net flux have been
shown to track the changes in OHC data
16,17
. is suggests that the
intrinsic precision of CERES is able to resolve the small imbalances
on interannual timescales
12,16
, thus providing a basis for constrain-
ing the balance of the measured radiation fluxes to time-varying
changes in OHC (Supplementary Information). e average annual
excess of net TOA radiation constrained by OHC is 0.6±0.4 Wm
–2
(90% confidence) since 2005 when Argo data
14
became available,
before which the OHC data are much more uncertain
14
. e uncer-
tainty on this estimated imbalance is based on the combination of
both the Argo OHC and CERES net flux data
16
.
1
Center for Climate Sciences, Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, California 91109, USA,
2
Institute for Atmospheric and Climate Science, ETH Zurich, Universitätsstrasse 16, CH-8092, Zurich, Switzerland,
3
Phyiscal Oceanography Department,
Woods Hole Oceanographic Institution, 266 Woods Hole Road, Massachusetts 02543, USA,
4
NASA Langley Research Center, 21 Langley Boulevard,
Hampton, Virginia 23681, USA,
5
Department of Atmospheric Sciences, University of Wisconsin, Madison, Wisconsin 80523, USA,
6
UK Met Office, FitzRoy
Road, Exeter, Devon EX1 3PB, UK. *e-mail: graeme.stephens@jpl.nasa.gov
PROGRESS ARTICLE
PUBLISHED ONLINE: 23 SEPTEMBER 2012 | DOI: 10.1038/NGEO1580
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