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Transcript
Geophysical Research Abstracts
Vol. 18, EGU2016-16529-2, 2016
EGU General Assembly 2016
© Author(s) 2016. CC Attribution 3.0 License.
Slab Ocean El Niño atmospheric feedbacks in Coupled Climate Models
and its relationship to the Recharge Oscillator
Tobias Bayr, Christian Wengel, and Mojib Latif
GEOMAR Helmholtz-Zentrum für Ozeanforschung Kiel, Maritime Meteorologie, Kiel, Germany ([email protected])
Dommenget (2010) found that El Niño-like variability, termed Slab Ocean El Niño, can exist in the absence
of ocean dynamics and is driven by the interaction of the atmospheric surface heat fluxes and the heat content
of the upper ocean. Further, Dommenget et al. (2014) report the Slab Ocean El Niño is not an artefact of the
ECHAM5-AGCM coupled to a slab ocean model. In fact, atmospheric feedbacks crucial to the Slab Ocean El
Niño can also be found in many state-of-the-art coupled climate models participating in CMIP3 and CMIP5, so
that ENSO in many CMIP models can be understood as a mixed recharge oscillator/Slab Ocean El Niño mode.
Here we show further analysis of the Slab Ocean El Niño atmospheric feedbacks in coupled models. The
BCCR_CM2.0 climate model from the CMIP3 data base, which has a very large equatorial cold bias, has an
El Niño that is mostly driven by Slab Ocean El Niño atmospheric feedbacks and is used as an example to
describe Slab Ocean El Niño atmospheric feedbacks in a coupled model. In the BCCR_CM2.0, the ENSO-related
variability in the 20◦ C isotherm (Z20), a measure of upper ocean heat content, is decoupled from the first mode of
the seasonal cycle-related variability, while the two are coupled in observations, with ENSO being phase-locked
to the seasonal cycle.
Further analysis of the seasonal cycle in Z20 using SODA Ocean Reanalysis reveals two different regimes
in the seasonal cycle along the equator: The first regime, to which ENSO is phase-locked, extends over the west
and central equatorial Pacific and is driven by subsurface ocean dynamics. The second regime, extending in
observations only over the cold tongue region, is driven by the seasonal cycle at the sea surface and is shifted by
roughly six months relative to the first regime.
In a series of experiments with the Kiel Climate Model (KCM) with different mean states due to tuning in
the convection parameters, we can show that the strength of the equatorial cold bias and the coupling strength
between the seasonal cycle of Z20 and ENSO are anti-correlated, i.e. a strong equatorial cold bias suppresses
recharge oscillator dynamics and enhances Slab Ocean El Niño atmospheric feedbacks, supporting the results
from the BCCR_CM2.0. This can be explained as with a stronger cold bias the second regime of the seasonal cycle
in Z20, which extends in observations only over the small cold tongue region, expands westward and becomes
more important, so that it decouples ENSO from the seasonal cycle in Z20. This has implications for some major
characteristics of the ENSO like the propagation of SST anomalies, the phase locking of SST to the seasonal
cycle, or the nonlinearity of ENSO.
Dommenget, D., 2010: The slab ocean El Niño. Geophys. Res. Lett., 37, L20701, doi:10.1029/2010GL044888.
——, S. Haase, T. Bayr, and C. Frauen, 2014: Analysis of the Slab Ocean El Niño atmospheric feedbacks in
observed and simulated ENSO dynamics. Clim. Dyn., doi:10.1007/s00382-014-2057-0.