Fig.
1. Global temperature (relative to 1880-1920 mean for each month) for
the 1997-98, 2015-16 and 2023-24 El Ninos. The impact of El Nino on
global temperature usually peaks early in the year (El Nino Peak Year)
following the year in which the El Nino originated.
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El Nino Fizzles. Planet Earth Sizzles. Why?
13 October 2023
James Hansen, Makiko Sato, Reto Ruedy, and Leon Simons
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Abstract.
September 2023 smashed the prior global temperature record.
Hand-wringing about the magnitude of the temperature jump in September
is not inappropriate, but it is more important to investigate the role
of aerosol climate forcing – which we chose to leave unmeasured – in
global climate change. Global temperature during the current El Nino
provides a potential indirect assessment of change of the aerosol
forcing. Global temperature in the current El Nino, to date, implies a
strong acceleration of global warming for which the most likely
explanation is a decrease of human-made aerosols as a result of
reductions in China and from ship emissions. The current El Nino will
probably be weaker than the 1997-98 and 2015-16 El Ninos, making current
warming even more significant. The current near-maximum solar
irradiance adds a small amount to the major “forcing” mechanisms (GHGs,
aerosols, and El Nino), but with no long-term effect. More important,
the long dormant Southern Hemisphere polar amplification is probably
coming into play.
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Fig. 2. Global temperature relative to 1880-1920 based on the GISS analysis.[1],[2]
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The September
global temperature anomaly leaped to more than +1.7°C relative to the
1880-1920 mean (Fig. 1). Public discussion has focused on the remarkable
magnitude of this monthly anomaly, which exceeds the prior warmest
September in the period of instrumental data by about +0.5°C; we will
comment on this extreme September anomaly below. However, the average
anomaly of the past 4 months (+0.44°C relative to the same months in
2015, the origin year of the 2015-16 El Nino) is probably more
important. If this relative anomaly is maintained through this El Nino
(through Northern Hemisphere 2024 spring) the peak 12-month mean global
warming will reach +1.6-1.7°C relative to 1880-1920. Decline of global
temperature following an El Nino peak is 0.2-0.3°C. Thus, if this El
Nino peak is as high as we project it will be, global temperature will
oscillate about the yellow region in Fig. 2. The 1.5°C global warming
level will have been reached, for all practical purposes. There will be
no need to ruminate for 20 years about whether the 1.5°C level has been
reached, as IPCC proposes. On the contrary, Earth’s enormous energy
imbalance (references 8, 13, 14 below) assures that global temperature
will be rising still higher for the foreseeable future.
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Fig.
3. Temperature in the tropical Pacific region used to define El Nino
strength. El Nino (La Nina) is nominally defined to occur when Nino 3.4
is > 0.5°C (< –0.5°C).
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These high
temperatures are occurring despite the fact that the current El Nino may
not even qualify as a “super” El Nino, comparable to those of 1997-98
and 2015-16. The Nino3.4 index (Fig. 3) at face value (upper Fig. 3) is
now about +1.5°C, but in assessing El Nino strength we should account
for the warming trend due to the net human-made climate forcing. The
simplest way to do that is to subtract the 1970-2010 trend of the
Nino3.4 temperature index, which is 0.1°C per decade (smaller than the
trend of global temperature, as expected due to polar amplification of
temperature change). With this detrending, the 1997-98 and 2015-16 El
Ninos seem to be equally strong. The Nino3.4 index (temperature anomaly
in a small region in the equatorial Pacific Ocean) is not a perfect
characterization of El Nino strength, however. As the maps in Fig. 4
show, the 1997-98 El Nino is actually stronger than the 2015-16 El Nino.
It’s too early to conclude the eventual strength of the 2023-24 El
Nino, but the early data (Fig. 4) do not suggest a very strong El Nino,
even though no trends have been subtracted in the data shown in Fig. 4.
Recent NOAA NCEP (Chart 25) forecast[3] has the Nino3.4 index reaching
only ~1.5°C. The ensemble average of many models collected by the
International Research Institute (IRI) of Columbia University and shown
in NOAA Chart 24 has the peak warming at ~1.5°C for the statistical
models and ~2°C for the dynamical models. Levine[4] provides a useful
discussion of El Nino in general and the current situation in
particular. Within the next several months we will be able to accurately
assess the current El Nino.
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Fig.
4. Surface temperature anomalies during the past two “super” El Ninos
and the first four months of the current El Nino. No attempt is made to
remove the global warming trend, so the apparent strength of the more
recent El Ninos is exaggerated by an unknown amount.
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The two dominant global climate forcings –
by far – are human-made greenhouse gases (GHGs) and human-made aerosols.
Although GHG changes are monitored precisely (and thus the GHG climate
forcing can be accurately computed), the aerosol forcing is not
similarly available. Direct measurement of aerosol climate forcing
requires global monitoring of aerosol and cloud particle
microphysics[5] as the principal aerosol forcing is via the effect of
aerosols on cloud microphysics. Aerosol and cloud particle monitoring of
sufficient accuracy would require high precision data for the
polarization of reflected sunlight and a high precision infrared
spectrometer in near-polar orbit. Although such measurements are
possible,[6] it was decided not to include them in NASA’s Earth
Observing System, and thus the aerosol forcing must be estimated as well
as possible from existing data in combination with aerosol and cloud
modeling.
An indirect indication of global aerosol forcing will be provided by the
magnitude of global warming at the peak of the current El
Nino,[7] which is expected to occur next Northern Hemisphere Spring,
i.e., within the next six months. A moderate reduction of global aerosol
amount has occurred due to reduced aerosol precursor emissions in China
and from ships.[8] Thus, instead of aerosols reducing the rate of
global warming, aerosol changes now should be adding to global warming.
We attribute the lack of an apparent acceleration of global warming to
date to the effect of the recent prolonged La Nina. When the Nino3.4
record is corrected (Fig. 3, lower part) to remove the trend caused by
global warming, it becomes apparent that the recent La Nina was strong,
comparable to those of the mid-1970s and late 1990s. The El Nino thus
provides a crude measure of possible acceleration of global warming. A
50% acceleration of the long-term (1970-2010) global warming rate
(0.18°C per decade) is shown by the lower edge of the yellow region in
Fig. 2, while the upper edge is 100% acceleration to 0.36°C per decade.
Although it is difficult to predict future aerosol climate forcing, we
expect a continual decline of the aerosol effect because of desire to
reduce particulate air pollution, which causes several million deaths
per year. Much of the aerosol pollution arises from fossil fuels, so, as
the world moves to clean energies, aerosol amounts should decline and
unmask the GHG warming that had been compensated by aerosol cooling. (We
long ago[9] described this aerosol cooling as a Faustian bargain, and
later[10] discussed it in more detail.) Thus, for the next few decades –
barring purposeful actions to reduce Earth’s energy imbalance – we
expect the global warming rate will be accelerated to at least the rate
(50% increase) of the lower boundary of the yellow area.
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Other than GHGs and aerosols, the climate
forcing most likely to affect current global warming is solar
irradiance, which is presently nearing the maximum of the ~11-year solar
cycle (Fig. 5). Because of the oscillatory nature of the solar forcing
and its limited magnitude (half-amplitude ~ 0.1 W/m2) it is a
minor but not negligible forcing. Hypotheses that the solar forcing
could be amplified by some feedback can be tested by searching for an
effect of the solar cycle on Earth’s energy imbalance (EEI). Fig. 6,
comparing solar irradiance and EEI, presents little evidence in favor of
a substantial solar effect. There is a very weak correlation (maximum
~0.3) with the irradiance leading EEI by 30-45 months (the expected
sense), but the record is too short and effect too small to suggest any
role for the Sun other than that expected for its very small irradiance
variation.
The Hunga Tonga volcanic eruption in early 2022 also affects EEI in the past two years. Jenkins et al.[11] estimate that water vapor injected into the stratosphere caused a small warming forcing (+0.12 W/m2), but Schoeberl et al.[12] found
that the cooling effect of stratospheric aerosols injected by Hunga
Tonga yielded a net cooling effect, with forcing peaking in mid-2022 at
about –0.5 W/m2. By today, the Hunga Tonga forcing is small and declining.
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Fig. 6. Solar irradiance variations (see Fig. 4) and Earth’s energy imbalance.[13],[14]
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The important point is that there are two
large human-made climate forcings: GHGs and aerosols. The aerosol
forcing is poorly understood. The magnitude of global warming during a
large El Nino provides a measuring stick that can help us detect
acceleration of global warming, but we need more detailed, quantitative
information on aerosol effects. The sharp change in aerosol emissions
caused by changes in regulations on the sulfur content of ship fuels
provide an opportunity to evaluate the aerosol effect, especially in the
North Pacific and North Atlantic regions of heavy ship traffic.
One final comment. The discussions of the remarkable September global
warming have noted that much of the warming is associated with an
extreme warming anomaly over Antarctica, with the suggestion that this
warming is a weather effect that will disappear. While it is true that
Antarctic temperature fluctuates greatly from month to month, we note
that there is a latent southern Hemisphere polar amplification of
warming that has long been dormant, as Southern Hemisphere sea ice cover
has been relatively constant for several decades. The recent decline of
sea ice area may be an indication that, averaged over weather,
Antarctica will become a more important contributor to global
temperature change.
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[1] Lenssen NJL, Schmidt GA, Hansen JE et al. Improvements in the GISTEMP uncertainty model, J Geophys Res Atmos 2019; 124(12):6307-26
[2] Hansen J, Ruedy R, Sato M et al. Global surface temperature change. Rev Geophys 2010; 48:RG4004
[3] https://www.cpc.ncep.noaa.gov/products/analysis_monitoring/lanina/enso_evolution-status-fcsts-web.pdf
[4] Levine, A, What is a strong El Nino?, The Conversation, PhysOrg, 12 October 2023.
[5] Mishchenko MI, Cairns B, Kopp G et al. Accurate monitoring of terrestrial aerosols and total solar irradiance: Introducing the Glory mission. Bull Amer Meteorol Soc 2007; 88:677-691
[6] Hansen J, Rossow W, Fung I. Long-term monitoring of global climate forcings and feedbacks. Washington: NASA Conference Publication 3234, 1993
[7] Grantham, J., The Race of Our Lives Revisited, GMO White Paper, August 2018.
[8] Hansen J, Sato M, Simons L et al. Global warming in the pipeline. Submitted to Oxford Open Climate Change, we expect the revised version of this paper to be published soon.
[9] Hansen JE, Lacis AA, 1990: Sun and dust versus greenhouse gases: An assessment of their relative roles in global climate change. Nature, 346, 713-719, doi:10.1038/346713a0.
[10] Hansen J. Storms of My Grandchildren. ISBN 978-1-60819-502-2. New York: Bloomsbury, 2009
[11] Jenkins S, Smith C, Allen M et al. Tonga eruption increase chance of temporary surface temperature anomaly above 1.5°C. Nature Climate Change 2022; 13:127-9
[12] Schoeberl M, Schoeberl MR, Wang Y, et al. The estimated climate impact of the Hunga Tonga-Hunga Ha’apai eruption plume 1. Geophys Res Lett (in press).
[13] Loeb NG, Johnson GC, Thorsen, TJ et al. Satellite and ocean data reveal marked increase in Earth’s heating rate. Geophys Res Lett 2021; 48:e2021GL093047
[14] von Schuckmann K, Cheng L, Palmer MD et al. Heat stored in the Earth system: where does the energy go?, Earth System Science Data 2020; 12:2013-41
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