SST predictions with an intermediate coupled model of the tropical Pacific.
contributed by Boris Dewitte1, Dasha Gushchina 2, Yves duPenhoat 1 and Rodrigo Abarca del Rio3
1LEGOS/CNES/IRD 14 Av. E. Belin, 31401 Toulouse Cedex
4, France
2Meteorological Department, Geographical Faculty,
Moscow State University, Vorobyevy gory, Moscow, 119899, Russia
3 DEFAO, University of Concepcion, Casilla 160-C,
Concepcion, Chile
Forecasts of the tropical
Pacific SST are presented here using two intermediate coupled models. The
oceanic component consists in a three baroclinic mode ocean and the mixed layer
model differs from the Cane and Zebiak (1987) model in the parameterization of
the vertical advection terms and the basic state (cf. Dewitte, 2000). The
atmospheric component is either a statistical atmospheric model based on the
singular value decomposition (SVD) of observed sea surface temperature (SST)
and wind stress anomalies (see Périgaud et al., 2000) or a Gill(1980)'s
dynamical tropical atmosphere. Initial conditions for the prediction runs are
produced in a coupled mode by nudging the observed winds (FSU winds for the
period 1961-1992, ERS1-2 winds from may 1992 until september 2000, QuikSCAT
winds from october 2000) to the simulated winds as in Chen et al. (1995). The
skill of the models for the NINO3 SST index over various periods and for the
1997-1998 El Niño is presented in Dewitte et al. (2002).
Figure 1 shows model predicted SST
and wind stress anomalies in the tropical Pacific for the next four seasons in
the case of the statistical atmosphere. These are ensemble averages of 12
forecasts started from Mar-Apr-May 2004 conditions. For producing the initial
conditions of the individual forecasts, random noise was added to the system
with an approach similar to Kirtman and Schopf (1998).
The model using the statistical atmosphere is predicting slightly cold
conditions for 2004, whereas the model using the dynamical atmosphere (figure 2) predicts slightly warm conditions
developing from the Sep-Oct-Nov 2004 season.
Caveat: The forecasts shown above are experimental in nature. The
reader is forewarned that the methods/forecasts are new and subject to future
change and improvement.
References:
Chen, D., S. E. Zebiak, A. J. Busalacchi, and M. A. Cane, 1995: An
improved procedure for El Niño forecasting: Implication for predictability. Science,
269, 1699-1702.
Dewitte B., 2000: Sensitivity of an intermediate coupled
ocean-atmosphere model of the tropical Pacific to its oceanic vertical
structure. J. Climate, 13, 2363-2388.
Dewitte B., D. Gushchina, Y. duPenhoat and S. Lakeev, 2002: On the
importance of subsurface variability for ENSO simulation and prediction with
intermediate coupled models of the Tropical Pacific: A case study for the
1997-1998 El Niño. Geoph. Res. Lett., 29 (14). (15 jul. 2002)
Gill, A., Some simple solutions heat-induced tropical circulation. Q.
J. R. Meteorol. Soc., 106, 447-462, 1980.
Kirtman, B. P. and P. S. Schopf, 1998: Decadal variability in ENSO
predictability an prediction, J. Climate, 11, 2804-2822
Périgaud C. C. Cassou, B. Dewitte, L.-L. Fu and D. Neelin, 2000: Using
data and intermediate coupled models for seasonal-to-interannual forecasts. Mon.
Wea. Rev., 128, 3025-3049.
Zebiak, S. E. and M. A. Cane, 1987: A model El Niño-Southern
Oscillation. Mon. Wea. Rev., 115, 2262-2278.
Figure Captions:
Fig. 1: model forecast of
tropical Pacific SST (°C) and wind stress (Dyn/cm2) anomalies for
JJA 2004, SON 2004, DJF 2004/2005 and MAM 2005. Each forecast is an ensemble
average of 12 sets of prediction runs initialized from wind forced model
outputs perturbated by random noise. Observed data through 28th of
May 2004 was used to produce the forecast. Contour interval 0.5°C. Regions with
SSTA amplitude larger than 0.5°C (lower than -0.5°C) are in yellow-orange
(blue). The longuest wind stress arrow on each map corresponds to the value
indicated on the right hand side. Only wind stress anomalies for which wind
modulus is larger than 0.1 Dyn/cm2 are plotted.
Fig.2: same as Fig.
1 but for the coupled model using the dynamical atmosphere.