Earth’s east–west albedo symmetry
Article
Earth’s east–west albedo symmetry
https://doi.org/10.1038/s41586-026-10624-2
Jianhao Zhang1,2 ✉, Jake J. Gristey1,2,3 & Graham Feingold2
Received: 25 November 2025
Accepted: 5 May 2026
Published online: xx xx xxxx
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Earth’s albedo is fundamental to the planetary energy budget1. The Northern
Hemisphere (NH) and Southern Hemisphere (SH) contribute essentially equally to
the planetary albedo—a remarkable yet puzzling phenomenon known as hemispheric
albedo symmetry1–6. Although such symmetry is rare, it is not unique7. Nevertheless,
other symmetry pairs have remained unexplored, despite their potential to illuminate
possible causes of albedo symmetries and implications for the planetary energy
budget. Using a 25-year satellite record, here we show that Earth also exhibits a unique
and persistent east–west (E–W) albedo symmetry: the 27° E meridian divides the
planet into an Eastern Hemisphere (EH) and a Western Hemisphere (WH) that reflect
nearly identical amounts of sunlight. In contrast to the NH–SH symmetry, the EH–WH
symmetry encapsulates a distinctive ‘triple symmetry’ in which clear-sky albedo,
cloud radiative effect and open-ocean fraction all exhibit hemispheric symmetry
around this meridian. This EH–WH symmetry arises from greater high-cloud reflection
in the EH balancing greater low-cloud reflection in the WH. Furthermore, interannual
variability in the EH–WH symmetry tracks the phase of the El Niño–Southern
Oscillation (ENSO), indicating a potential connection to general circulation. This
discovery of the EH–WH albedo symmetry and its emergence as a triple symmetry
provides a reduced degree-of-freedom constraint for Earth system models (ESMs)
and stresses the critical nature of continued Earth radiation budget observations
under a rapidly changing climate.
The Earth reflects about 29% of the incoming solar radiation back
to space, an intrinsic property of a planet known as the planetary
albedo1. An intriguing observation has emerged since spaceborne
monitoring of Earth’s radiative fluxes became available half a century
ago: the NH and SH reflect almost identical amounts of sunlight1–4,7–9.
Although this symmetry is known to arise from a cloudier SH balancing more reflective clear skies in the NH1,5,8,10, the lack of satisfactory
mechanistic explanations for how the north–south (N–S) symmetry
is maintained leaves open the possibility of a coincidence, and the
N–S symmetry remains a mystery6,8. This possibility is further fuelled
by the fact that observations may now suggest a departure from N–S
symmetry11–13.
Given that the Earth is approximately spherical, it is unsurprising that
one can divide it into two non-overlapping hemispheres that reflect
equal amounts of sunlight. However, the chance of achieving such a
hemispheric symmetry within 0.1 W m−2 is less than 3% (ref. 7), making
the hemispheric symmetry unlikely to be coincidental. An unexplored
question is what we can learn from these rare hemispheric pairs in
which symmetry holds, insights that could be fundamental to understanding the Earth’s climate system. Similarities or differences across
symmetry pairs could shed light on the underlying couplings among
Earth system components.
This work presents the first investigation of the Earth’s hemispheric
albedo symmetry as a function of longitude. We divide the planet into
EHs and WHs at every longitudinal great circle, with one-degree increments, and identify 27° E (with 153° W completing the great circle) as
the unique meridian that produces an E–W albedo symmetry using
25 years of satellite-measured top-of-atmosphere (TOA) shortwave
(SW) fluxes. The finding of the E–W symmetry at 27° E is notable for
its persistence and the fact that it represents the only longitudinal
divide yielding such balance. Moreover, it coincides with the meridian that separates the Earth into two hemispheres containing almost
the same amounts of ice-free ocean. Put differently, the ratio of land
to ocean correlates strongly with the reflected solar flux in the two
hemispheres, a feature in strong contrast to the N–S symmetry. In a
hypothetically cloud-free world, this correspondence might not be
surprising, given the contrast in surface reflectivity between land and
ice-free ocean. However, for the cloudy planet we inhabit, the persistence of this symmetry becomes nontrivial, underscoring the need
to understand the role of clouds in maintaining the observed E–W
symmetry.
Using more than two decades of Clouds and the Earth’s Radiant
Energy System (CERES) observations14–17, we show that the E–W symmetry at 27° E arises from a high-cloud-dominated EH balancing a
low-cloud-dominated WH, and from an EH with more reflective oceanic
and ice-covered regions balancing a WH with more reflective ice-free
continental regions. This E–W symmetry, coinciding with an even
divide of hemispheric ice-free-ocean fractions and a near symmetry
in cloud radiative effect (CRE)—a triple symmetry—is not captured by
climate models. We find a strong correlation between the interannual
variability of the E–W hemispheric albedo symmetry and the phase of
ENSO, suggesting that large-scale atmospheric circulation, particularly
the Walker circulation, may play an important role in maintaining this
symmetry.
1
Cooperative Institute for Research in Environmental Sciences (CIRES), University of Colorado Boulder, Boulder, CO, USA. 2Chemical Sciences Laboratory, National Oceanic and Atmospheric
Administration (NOAA), Boulder, CO, USA. 3Laboratory for Atmospheric and Space Physics (LASP), University of Colorado Boulder, Boulder, CO, USA. ✉e-mail:
Nature | www.nature.com | 1
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Longitude (°)
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−10.0
−1
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27° E
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−0.15
ΔR
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−7.5
N–S symmetry (equator)
E–W symmetry (27° E)
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ΔCRE
Starting year
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−0.10
ΔRclr
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−5.0
c
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−0.05
Symmetry
longitude (° E)
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20.0
26 27 28
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25.0
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Median
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0.15
Consecutive
years averaged
7.5
Mean
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20
b
0.20
ΔR (W m−2)
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ΔO (EH minus WH)
EH minus WH (W m−2)
a
Symmetry longitude (° E)
Article
Year
Fig. 1 | Demonstration of Earth’s E–W hemispheric albedo symmetry and
its persistence. a, 25-year mean differences in reflected SW radiation based
on CERES EBAF51 as a function of longitude and coloured by the difference in
ice-free-ocean fraction (ΔO ) between the EH and the WH (EH minus WH). All-sky
reflection difference (ΔR ) is shown by circles, clear-sky reflection difference
(Δ R clr ) is shown by upward triangles and CRE difference (ΔCRE) is shown by
downward triangles. Values at 27° E are highlighted with black outlines. An
approximate triple symmetry at 27° E, for O , R clr and CRE, is a unique feature
of the E–W symmetry (...truncated)