U.S. Dept. of Commerce / NOAA
/ OAR / GFDL
*Disclaimer
4. EXPERIMENTAL PREDICTION
GOALS
To develop methods of stochastic-dynamic prediction capable of extracting
as much useful forecast information as possible from numerical prediction
models given imperfectly observed initial conditions.
To develop and improve numerical models of the atmosphere-ocean-land
system in order to produce useful forecasts with lead times of several
weeks, months, seasons or years.
To understand the limits of predictability of the ocean-atmosphere
system with emphasis on quantifying the amount of useful forecast information
that could be available at lead times of several weeks, months, seasons
or years.
To develop methods for the assimilation of observations into dynamical
models in order to improve predictions of the ocean and atmosphere.
4.1 ATMOSPHERIC AND OCEANIC PREDICTION
AND PREDICTABILITY
ACTIVITIES FY00
4.1.1 Ocean Model Development
for Seasonal/Interannual Prediction
S. Griffies A.
Rosati
M. Harrison
The advent of more
powerful computers will permit the next generation of ocean climate models
to have a grid resolution necessary for studies of seasonal-to-interannual
prediction. Consequently, over the past year the ocean model development
efforts of the Climate Dynamics group have been closely coordinated with
members of the Experimental Prediction group. The past year has seen prototype
studies of ocean grid resolution and ocean parameterizations which are
useful to both groups. Most notably, such work expands the domain of the
experimental prediction group's ocean model into the Arctic.
This development
work represents part of a multi-year effort aimed at enhancing the realism
of GFDL's ocean simulations (1535, 1536, 1676). In particular, this new
ocean model will facilitate study of longer term phenomena, such as decadal
fluctuations of ENSO and variations in the thermohaline circulation.
4.1.2 Coupled Model
Development for Seasonal/Interannual Prediction
J. Anderson A.
Rosati
C.T. Gordon J.
Sirutis
S. Griffies R.
Smith
R. Gudgel W.
Stern
S. Klein M.
Winton
M. Harrison B.
Wyman
J. Ploshay
A new coupled model
to be used for seasonal/interannual forecasting is under development. The
configuration of the atmospheric component has not yet been determined.
However, using Bombay release versions of the Flexible Modeling System
(FMS) (1.3.3), an atmospheric model has been assembled with the following
features: N45L18 B-grid dynamical core, 4th-order advection, Klein predicted
clouds (3.2.4), diurnal variation of radiation, and RAS (Relaxed Arakawa
Schubert) convection. The ocean component is MOM3 and is also used as the
base model for a comparison project with the International Research Institute
for Climate Prediction/Applied Research Centers (IRI/ARCS). This model
is nearly global (no Arctic Ocean) with one degree resolution increasing
to one-third degree meridional resolution within ten degrees north and
south of the equator. The vertical resolution is 40 levels with a constant
10 m resolution to 200 m. The physical parameterizations include K-Profile
Parameterization (KPP) vertical mixing, Smagorinsky viscosity (1720), Gent-McWilliams
(GM) diffusion for horizontal mixing (1536), and an explicit free surface.
The coupling between component models uses the FMS coupling framework (1.1.3).
Modifications to pass fluxes to MOM and sea surface temperatures (SSTs)
to the atmosphere, required because MOM3 is not a compliant FMS component
model, have been completed. Preliminary coupled forecast experiments using
this system are being run, although only rudimentary tuning has been done.
Early indications are that the mechanics of the coupling are working, although
considerable tuning will be required to produce acceptable simulations
and predictions.
4.1.3 Statistical
Atmospheric Model Development
A statistically-based
atmospheric model has been developed using SST anomalies as predictors
and ocean surface fluxes of heat, momentum, and freshwater as predictands.
The model was initially developed using the National Centers for Environmental
Prediction (NCEP) and European Centre for Medium Range Weather Forecasting
(ECMWF) Reanalyses and the GFDL Atmospheric Model Intercomparison Project
(AMIP) 2 model used for seasonal to interannual prediction. The model is
capable of generating sustained oscillations when coupled with an ocean
model without additional tuning. Considerable differences have been observed
between atmospheric products (1624, na); for instance, the statistical
version of the ECMWF Reanalysis model yielded sustained coupled oscillations,
while the GFDL statistical model was highly damped when coupled to the
ocean model. Subcriticality in the coupling between atmosphere and ocean
resulted in diminished forecast skill, as measured by Niño3 SST
correlation and RMS error.
4.1.4 Sensitivity
to Horizontal and Vertical Resolution in Atmospheric Models
C.T. Gordon J.
Sirutis
R. Gudgel W.
Stern
A. Rosati B.
Wyman
The impact of vertical
and horizontal resolution in the B-grid atmospheric model (1.2.4) is under
investigation in an attempt to determine the required resolution for improved
coupled predictions. Initial results are focusing on the quality of simulations
of basic atmospheric quantities. As an example, Fig. 4.1 shows the 1980-1981
mean winter and summer zonal jets from the NCEP reanalysis, and corresponding
2-year integrations from N45L18, N45L30, and N90L18 model simulations.
Evaluation of many additional diagnostic quantities, aided by the capabilities
of the GFDL web-based diagnostic facility (6.4) will determine the most
cost-effective resolution.
4.1.5 Impact of Land
and Ocean Low-Level Tropical Clouds on ENSO Prediction
C.T. Gordon A.
Rosati
R. Gudgel
The role of tropical
land and ocean low-level clouds in the ability of a coupled atmospheric-ocean
general circulation model (AOGCM) to predict ENSO has been studied (nl)
through a set of ten 12-month model integrations. In the tropics, a strong
bias in a GFDL Experimental Prediction AOGCM is evident in the western
tropical Pacific, where overly strong convection diminishes the SST warm
pool, reducing the east-west SST gradient, and effectively weakening the
trade winds. This bias is exacerbated by the poor simulation of tropical
marine stratocumulus clouds (MSc) in the eastern equatorial Pacific, which
are essential to a proper SST annual cycle. The sensitivity of the AOGCM
simulation of the tropical circulation to prescribing low-level clouds
obtained from the International Satellite Cloud Climatology Project (ISCCP)
was studied. The results showed that the combined prescription of global
ocean and tropical land low-level clouds in the AOGCM resulted in the best
simulation of the Walker circulation. The improved tropical circulation
was accompanied by an improvement in the one-year prediction of ENSO by
the AOGCM. It was determined that the combination of more realistic MSc
in the eastern tropical Pacific and more realistic tropical land surface
heating led to the improvements.
The top panel
in Fig. 4.2 depicts ENSO hindcast skill in the Niño3 region. The
skill scores show that the addition of the low-level ISCCP clouds over
the oceans alone (CMIO) has indeed resulted in an improvement in model
skill compared to the fully predicted cloud
experiment (CM). The CMIOL experiment (prescribed clouds over both ocean
and land) shows even more skill for the entire 12-month period. The experimental
rms errors, shown in the middle panel of Fig. 4.2, indicate that only the
CMIOL experiment separates itself from the other experiments as having
reduced error. It follows that although the ocean low-level clouds are
assisting the CMIO experiment to simulate the correct sign of the SST anomaly,
these clouds alone are not sufficient to simulate the amplitude of the
ENSO events. The lower panel of Fig. 4.2 shows that the CMIOL experiment
has a more realistic simulation of precipitation than the other experiments,
though it does err on the side of underpredicting precipitation.
Multi-year simulation
experiments with low (as well as multi-level) ISCCP cloud fractions and
optical depths were performed with a newer version of the coupled model.
However, relative to results obtained with the previous model (1719), the
SSTs in the tropical Pacific cooled a few degrees and displayed much weaker
interannual variability in the equatorial belt. Moreover, what variability
remained was not ENSO-like in character, e.g., was not linked to
a delayed oscillator mechanism. On the contrary, it appeared to be driven
by westward propagating variations in surface heat flux associated with
the ISCCP low clouds in the eastern tropical Pacific. This behavior is
presumably due to one or more new features of the new coupled model: MOM3
instead of MOM2, RAS with a re-tuned threshold parameter instead of the
full Arakawa-Schubert convective parameterization, variable high cloud
emissivity, diurnally-varying radiation, and elimination of the 10% proportional
surface evaporative flux correction.
4.1.6 Atmospheric
Model Predictability: Top of the Atmosphere Radiation Budget
L. Donner W.
Stern
C.T. Gordon
Bruce Wielicki of
NASA/Langley is comparing several AGCM (Atmospheric GCM) simulations of
the earth's tropical radiation budget to Earth Radiation Budget Experiment
(ERBE) and to Clouds and the Earth's Radiant Energy System (CERES) satellite
observations. GFDL has provided results that are relevant to evaluating
the ability of GCMs to simulate interannual variability as well as secular
trends. Two sets of AGCM runs with specified SSTs from 1997/1998 were analyzed:
the single AMIP 2 run; and a 10-member ensemble of 28-month Monsoon Modeling
Intercomparison Project (MMIP) integrations started from the AMIP 2 run.
Both the phase
and amplitude of the outgoing longwave radiation (OLR) and net absorbed
shortwave anomaly fields (calculated with respect to the 1985-1989 monthly
and 2-month means) verified extremely well compared to observations. Results
from the 10 MMIP ensemble members indicated that the El Niño signal
was very robust. In fact, the "GFDL-EP" "model (in contrast to the GFDL
climate model) was among the top performers. These excellent interannual
variability results may be attributed to the ability of the diagnostic
cloud parameterization scheme to discriminate between anvil cirrus and
non-anvil cirrus clouds in terms of cloud optical depth and emissivity.
On the other hand, none of the models captured the apparent trend in global
mean OLR suggested by a comparison of the CERES observations with earlier
ERBE observations.
4.1.7 Impact of MJO/WWB
in the Far Western Equatorial Pacific on ENSO Forecasts
The influence of
the Madden-Julian Oscillation (MJO) on ENSO is an intriguing and controversial
issue. Extraordinary MJO events coincided with the onset of the 1997/1998
warm event, which was unusual in its magnitude and rapidity of onset. In
order to gain a quantitative understanding of the role of MJO and westerly
windburst (WWB) events in ENSO prediction, a hybrid coupled model (HCM)
forecast system was applied. The ocean model is MOM3 with 1 degree
zonal and 1/3 degree meridional resolution. The statistical atmosphere
(4.1.3) is based on ECMWF reanalysis surface windstress, evaporation, and
radiation fluxes regressed to SST anomalies. The experimental design included
ocean initial conditions from the GFDL ocean data assimilation system and
control forecasts using the HCM for the 1980-1998 period. Another experiment
was run using the observed wind time series within a region bounded by
120°E-165°E and 5°S-5°N. This case gave much better predictions
of the large events in 1982-1983, 1988, and 1997, resulting in significantly
better skill scores. The 1982 and 1997 El Niños were amplified by
wind events from the preceding March. While the model predicted these warm
events without the patch winds, the amplitude was significantly underestimated.
The wind events were found to trigger ocean Kelvin waves which result in
deepening of the thermocline in the Eastern Pacific with subsequent SST
warming and amplification by coupled interactions.
4.1.8 Interaction
of MJO and Tropical Storms
A number of observational
studies have indicated the existence of a relationship between the frequency
of tropical storm occurrence and the MJO. Tropical storm formation appears
to be enhanced during the convectively active phase of the MJO. Data from
a 20-year AMIP 2 run made with the experimental prediction AGCM have been
analyzed and indicate that there is indeed a relationship. For 16 of the
19 years analyzed, over 50% of the tropical storms in the model formed
during the convectively active phase of the MJO; for 7 of the 19 years,
more than 70% formed during the convectively active phase of the MJO. This
relationship was strongest in the west Pacific during the 1980s. During
the 1990's the signal was stronger in the east Pacific and the Atlantic.
During El Niño years the relationship seems to be weak or non-existent.
The MJO also has an impact on the intensity of tropical storms in the model.
During the 19 years analyzed, 75% of the tropical storms that reached hurricane
intensity (maximum winds exceeding 75 mph) occurred during the convectively
active phase of the MJO. In 7 of the 19 years, all of these "hurricanes"
formed during the convectively active phase of the MJO.
4.1.9 The Nature
and Predictability of Tropical Intraseasonal Oscillations
R.Smith D.
Waliser*
W. Stern
*Marine Sciences Research Center, SUNY
Results from both
AMIP (1540) and coupled GCM integrations are being used to investigate
tropical intraseasonal oscillations (TIO). As part of the Monsoon Modelling
Intercomparison Project, a comparison of TIO/MJO behavior in the 1982-1983
and 1997-1998 ENSOs was performed using 10-member ensembles of AGCM integrations
forced by observed SSTs. Longitude-time plots and power spectra indicate
a difference in MJO behavior between the onset and mature phases of both
ENSO events. Statistical tests indicate that some of the MJO interannual
variability is significant, especially in the west-central equatorial Pacific
Ocean. Considerable TIO activity is also seen in the Asian monsoon region
and appears to be associated in part with northward propagation from the
equatorial Indian Ocean. An association between equatorial MJO activity
and Monsoon rainfall intensity is being sought.
Results from
Coupled Model Ensemble Prediction (CMEP) coupled GCM are being analyzed
to better understand TIO as a coupled atmosphere-ocean phenomenon. Fig.
4.3 shows evidence of a robust TIO in the model using the first extended
EOF of bandpassed (20-100 day) 200 hPa velocity potential. This EOF compares
favorably to those from the NCEP/NCAR reanalysis, but it is stronger. By
forcing the atmospheric AGCM with SSTs generated by the CGCM and comparing
these results to those obtained using a weakly interacting slab mixed-layer
ocean, a better understanding will be gained of how interactive ocean processes
impact the behavior of TIO.
4.1.10 Coupled Model
Potential Predictability
To increase understanding
of the prediction and predictability (1539) of the coupled GCM and the
coupled atmosphere-ocean system (ke), an ensemble of one-year forecasts
was run with members differing only in small perturbations to the 850 mb
temperatures in the atmospheric initial conditions. These results complement
earlier results from the CMEP experiments in which somewhat larger initial
condition perturbations were used. The spreads in the predicted SST anomalies
over the east-central Pacific Ocean are as large as in the forecasts produced
from initial conditions with much larger differences. For several of the
years investigated, SST spreads of several degrees can appear in the tropical
Pacific within a few months of the start of the forecast. This implies
that predictions of the thermal structure of the tropical Pacific cannot
be viewed as deterministic, even for lead times as short as one or two
seasons, at least for certain ocean initial conditions.
4.1.11 Indian Ocean
Variability
M. Harrison D.
Sengupta
A. Rosati
For the tropical
Pacific and Atlantic Oceans, internal modes of variability that lead to
climatic oscillations have been recognized, but in the Indian Ocean a similar
interannual climate variability caused by air-sea interaction has not yet
been found. However, recent observational analyses have suggested that
the interannual variability of the Indian Ocean consists of a dipole mode
in SST. These analyses further argue that the dipole mode is independent
of ENSO and is the result of internal dynamics. The dipole mode has important
implications for climate variability, as the shift of the convergence zone
leads to floods in east Africa and drought in Indonesia. A 1/4 degree ocean
model that covers the Indian Ocean basin was used to simulate the ocean
during 1997/1998. Preliminary results indicate the importance of both the
ocean dynamics and surface fluxes in the evolution of this mode. Fig. 4.4
shows the large subsurface temperature anomalies for November 1997 associated
with the dipole mode. Investigations of the sensitivity to various forcing
products and heat flux formulations are underway. These results are to
be compared to the GFDL ocean data assimilation for verification and understanding.
PLANS FY01
A key focus will
be on developing the components of a coupled forecast system that will
produce simulations and coupled predictions that are superior to those
that were available from the models used for seasonal prediction experiments
in the past five years. Initial efforts will focus on development of improved
individual component models, particularly for the atmosphere. Model resolution,
the choice of physical parameterizations, and the tuning constants available
in existing parameterizations are all candidates for change. A coordinated
diagnostic effort making use of new tools available at GFDL (6.4) along
with the capabilities of the FMS (Section 1) are expected to facilitate
model improvements. As component model improvements occur, they will be
tested in a fully-coupled model with a final goal of producing an improved
coupled model.
MOM4's diagnostic
capabilities and subgrid scale parameterization suite will be expanded
and MOM4 will become the ocean model of choice for coupled model development.
As improved coupled
models are developed, they will be integrated for several decades and used
to produce ensembles of forecasts from 1980-2000 to assess ENSO forecast
skill. The primary focus will be on the tropical circulation and the use
of physically based metrics for evaluating model performance. Among the
metrics are: ENSO variability and forecast skill; MJO; monsoon circulation;
tropical storm frequency and distribution; and precipitation patterns.
The Hybrid-Coupled
Model work will be extended to make additional comparisons between atmospheric
models developed at GFDL and the IRI/ARCS community. An evaluation will
be made of the relative merits of an anomaly coupled forecast system versus
a fully coupled system in the context of ENSO prediction; i.e.,
are there significant and predictable air-sea interactions which are not
captured by a diagnosed linear relationship to SST in any of the atmospheric
models considered ?
Further work
using the Hybrid Coupled Model will focus on trying to gain an understanding
of the relation between the ocean state and its response to MJO/WWB events.
The impact of an event and its relation to the seasonal cycle will be investigated.
The ability to
perform integrations with ISCCP low and/or multi-layer cloud fractions
and cloud optical depths will be added to the coupled FMS model, and reference
integrations with ISCCP low clouds will be performed.
An analysis will
be performed of the sensitivity of the interannual variability (as well
as the climatology) of the top of the atmosphere earth radiation budget
in the FMS model to the diagnostic and prognostic cloud parameterizations.
Many aspects
of the onset and development of the Indian Ocean dipole mode remain to
be investigated. Some of the questions to be studied are: Is there a preferred
background state? Are there regime shifts that account for why there was
no dipole in the 1980s but two in the 1990s? Is the dipole a coupled mode?
How does it grow and decay? Is there a possible relationship with ENSO?
4.2 DATA ASSIMILATION
ACTIVITIES FY00
4.2.1 Ensemble Adjustment
Filter
An established theory
(1658) exists for generating an estimate of the complete probability distribution
of the state of a model given a set of observations. This non-linear filtering
theory unifies the data assimilation and ensemble generation problem that
have been key foci of prediction and predictability research for numerical
weather and ocean prediction applications. A novel Monte Carlo approximation
to the fully non-linear filter has been developed and applied in perfect
model experiments in a low order model, a non-divergent barotropic model
in both perfect model and real data applications, and in a dry global primitive
equation model. This ensemble adjustment method is able to produce assimilations
with small ensemble mean errors while providing accurate measures of uncertainty
in the assimilated variables. The filtering method uses information from
an ensemble of model integrations to obtain an estimate of the covariance
between model state variables and observations. Each available observation
is then allowed to impact the prior distribution for each state variable
independently. However, the way in which the required product of the observational
error distribution and the prior state distribution is computed maintains
much of the information about covariances of the prior state variables.
The method is able to assimilate observations with a nonlinear relation
to model state variables, and has also been demonstrated to be effective
in using observations to adjust the value of unknown model parameters.
The method is shown to have significant advantages over four dimensional
variational assimilation in low order models (Fig. 4.5) and scales easily
to much larger applications.
4.2.2 Ocean Data
Assimilation
E. Galanti* R.
Pacanowski
R. Giering** A.
Rosati
M. Harrison E.
Tziperman
*The Weizmann Institute of Science
**NASA/Jet Propulsion Laboratory
A nearly global,
40 level ocean model (MOM3) with 1 degree zonal resolution and 1/3-1 degree
meridional resolution is being used for seasonal to interannual prediction
at GFDL. Ocean initial conditions are generated by a statistical interpolation
algorithm1 which
assimilates ocean profile data to depths of approximately 400 meters. These
ocean initial conditions and model configuration are being shared with
several collaborators as part of an IRI/ARCS forecasting effort.
Bi-weekly ocean
initial conditions have been distributed to groups at IRI, NCEP, COLA (Center
for Ocean, Land and Atmosphere studies), and NCAR for the period January
1980 through January 2000. The ocean model has been ported to parallel
computational platforms at the respective centers. Comparisons of forecasts
using identical ocean model and initial conditions but different atmospheric
models are being made.
Currently, monthly-averaged
data from the ocean analysis are available on the web (data1.gfdl.gov)
through interactive browsing software developed at PMEL by Steve Hankin.
In addition to the ocean assimilation, a simulation which does not make
use of subsurface data can be viewed in arbitrary latitude/longitude/depth/time
sections and downloaded for further analysis. Other ocean assimilation
products from Ming Ji and Dave Behringer at NCEP and Jim Carton at University
of Maryland are also available.
A four-dimensional
ocean assimilation system using a version of MOM4 coupled to a statistical
atmospheric model is currently being developed in collaboration with Eli Tzipermann
and Eli Galanti at the Weizmann Institute in Israel. The tangent linear
and adjoint versions of this model have been generated using a compiler
developed by Ralf Geiring.
4.2.3 Information
Content of Surface Pressure Observations
The ensemble adjustment
filter (4.2.1) has been applied in a dry global primitive equation model
to evaluate the information content of observations of surface pressure
in a perfect model experiment. A control integration of the model is used
to generate observations of surface pressure at a set of 600 randomly located
points on the surface of the sphere every six hours. Using only these observations,
the filter is able to reconstruct the structure of the free atmosphere
(Fig. 4.6). Without the impact of the surface pressure observations, the
ensemble
has an error doubling time of roughly 5 days and error saturates to
climatological values which are several orders of magnitude larger than
the RMS error of the assimilated ensemble mean after about 25 days. Applying
the adjustment filter allows much more efficient use of data than most
other known data assimilation methods and should improve our estimates
of the predictability of the atmosphere.
4.2.4 Targeted Observations
The "targeted observation
problem" tries to determine the location at which an additional observation
should be taken some time in the future in order to improve significantly
a forecast of some quantity at a time even further in the future. A number
of heuristic methods using operational ensemble predictions have been used
to attack this problem in recent years. The ensemble adjustment filter
method (4.2.1) for ensemble assimilation and prediction provides a framework
in which the targeted observation problem can be addressed. The filtering
method uses information from an ensemble of model integrations to obtain
an estimate of the covariance between model state variables and observations.
Each available observation is then allowed to impact the prior distribution
for each state variable independently. There is no reason that the impact
of observations must be limited to those available at the present time.
The impact of observations from previous times can also be computed in
this filter using the information available from the time history of the
ensemble of assimilations. Likewise, the impact of a hypothetical future
observation on a forecast even further in the future can also be approximated.
Initial results in a low order dynamical system have suggested that the
ensemble adjustment filter targeted observation method is significantly
superior to other methods currently available.
PLANS FY01
The ensemble adjustment
filter will be tested in high resolution primitive-equation models both
with and without comprehensive physical parameterizations. Further study
of the information content of surface pressure observations in more realistic
models should lead to an understanding of operational implications. Initial
application of the adjustment filter will be attempted in MOM. Strategies
for targeted observations in both low order and realistic models will be
refined.
Additional ocean
assimilation runs are being planned in collaboration with Mike Tippett
at IRI using a reduced empirical orthogonal function (EOF) space estimate
of model error. Forecasts using this technique will be compared to the
current ocean analysis.
Current
plans are to assimilate data from the TAO array in the equatorial Pacific
and wind data from the NCEP Reanalysis using the adjoint method. Working
in collaboration with Geiring, his compiler is being updated to be Fortran
90 compliant in concert with the latest developments of MOM4 (4.1.1). Developing
the ocean model and its adjoint compiler simultaneously is a key to this
effort.
4.3 OCEAN-ATMOSPHERE INTERACTIONS
J. Boccaletti G.
Philander
A. Federov B.
Winter
S. Harper A.
Wittenberg
ACTIVITIES FY00
Although there has
been considerable progress in our understanding of climate fluctuations
on seasonal, interannual, and decadal time-scales, a wide gulf still seems
to separate observational, theoretical, and modeling studies. Evidence
of this divide includes the following.
Theoretical studies
of El Niño focus on the natural modes of oscillation and, therefore,
take an eigenvalue approach. Measurements, on the other hand, pay essentially
no attention to the theoretical results and describe the development of
El Niño, of 1997 for example, in terms of westerly wind bursts that
initiate an event, treating the evolution as an initial value problem.
In a recent debate about the possible effect of global warming on El Niño,
the various arguments being presented all concern statistical issues; no
one is appealing to theoretical results to anticipate how global warming
will affect El Niño. Numerous groups are developing coupled ocean-atmosphere
GCMs and are simulating a bewildering variety of interannual oscillations.
It is not at all clear how the available theoretical results can contribute
to the development of realistic complex models. The remedy for these various
problems is a stability analysis that establishes how the properties of
the Southern Oscillation (its period, growth rate, etc.) depend on the
background state described in terms of readily measurable quantities, such
as the spatially averaged depth of the thermocline, the temperature difference
across the thermocline, and the time-averaged intensity of the trade winds.
Preliminary results from such an analysis have already been published (1710)
and a more detailed analysis has been completed (ab). This past year, attention
focused on application of these results to the interpretation of a realistic
simulation of oceanic conditions over the past fifty years with a GCM,
and to factors that can effect gradual (decadal) changes in the background
state. The distinctiveness of each El Niño was another topic that
was explored.
Decadal changes
in the depth of the thermocline and in the intensity of the time-averaged
zonal winds along the equator can account for certain observed changes
in the properties of El Niño from the 1960s to the 1980s. The period
of the Southern Oscillation, for example, increased from approximately
3 years to 5 years, but does not explain why El Niño was prolonged
and weak in 1992, but brief and intense in 1997. Westerly wind bursts near
the date-line appear to have played a central role in the development of
El Niño in 1997, but similar wind bursts were present on other occasions
and failed to generate any El Niño. Up to now, studies of these
wind bursts have concerned either their atmospheric aspects (whether they
are associated with certain sea surface temperature patterns, for example)
or the oceanic response they generate. Surprisingly, no one has investigated
the response of the coupled ocean-atmosphere system to these winds. A study
of the ocean-atmosphere interactions generated by westerly wind bursts,
by means of a simple Cane-Zebiak type coupled model, indicates that the
impact of the winds depends critically on the phase of the Southern Oscillation,
if one is present. A swinging pendulum subjected to blows at random times
is a good analogy. Westerly wind bursts can amplify El Niño enormously,
if they occur when the Southern Oscillation is in the early stages of its
El Niño phase, but have the opposite effect when they occur during
La Niña. This result has the important implication that, although
it should have been possible to anticipate El Niño of 1997 on the
order of a year in advance, it was not possible to anticipate its enormous
amplitude until the westerly wind bursts had actually occurred. Given this
role of unpredictable westerly wind bursts, El Niño has very limited
predictability. A long-term forecast can at best sound an alert that conditions
are ripe for an intense El Niño should the appropriate wind bursts
materialize. To make such a statement, the best quantity to monitor is
the available potential energy (1694) of the tropical Pacific which is
highly correlated with sea surface temperatures in the eastern tropical
Pacific, but has the advantage of being a global rather than a local quantity.
A realistic General
Circulation Model of the ocean (MOM), forced with the winds observed over
the tropical Pacific Ocean since 1950, provides data that permit a detailed
study of both gradual, decadal, and rapid event-to-event changes in the
properties of El Niño. Preliminary results indicate that the differences
between one event and the next can indeed be attributed to the impact of
random westerly wind bursts. Those winds contributed to the great intensity
of El Niño in both 1982 and 1997. A further contributing factor
was the change in the background state from the 1960s to the 1980s. The
easterly winds weakened over that period, and the thermocline gradually
deepened. This caused the structure of the Southern Oscillation to become
closer to that of the delayed oscillator in which sea surface temperature
variations in the eastern tropical Pacific are controlled mainly by vertical
movements of the thermocline in response to winds near the dateline. (During
the 1960s and 1970s, local winds in the eastern tropical Pacific had a
stronger influence on sea surface temperatures.) Thus, even if the structure
of westerly wind bursts remained unchanged over the decades, their impact
increased in the 1980s and 1990s because of the preferred mode during that
period.
The extent to
which oceanic exchanges between the tropics and subtropics contribute to
the decadal variations in the background state is a topic of continuing
interest. Experiments with a realistic oceanic GCM indicate that the disturbances
that reach the equator come predominantly from the Southern Hemisphere.
PLANS FY01
Studies planned
for the coming year include the use of an intermediate coupled ocean-atmosphere
model, composed of an oceanic GCM coupled to a statistical atmosphere in
which the winds correspond to that component of the observed winds correlated
with tropical sea surface temperature changes. The goal will be to explore
the validity of the stability analysis which was obtained by means of a
very simple coupled model with a great number of adjustable parameters
in a more realistic setting. The strategy will be to focus on certain extreme
situations where the differences between the possible modes are very large:
the delayed oscillator mode that is favored when the thermocline is deep
and the winds are intense, versus the local mode when the thermocline is
shallow. (In the local mode sea surface temperatures depend not on vertical
movements of the thermocline, but primarily on entrainment across the thermocline
and on zonal advection.) The coupled model will also be used to explore
how changes in the structure of the equatorial thermocline, induced by
tropical-subtropical exchanges, affect ocean-atmosphere interactions.
1. Derber, J.,
and A. Rosati, A Global Oceanic Data Assimilation System, Journal of
Physical Oceanography, 19(9), 1333-1347, 1989.
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