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chapter - Atmospheric and Oceanic Science

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Low-frequency variability<br />

In general, these patterns show robust (weak) <strong>and</strong> quite well (noisy) spatial structure<br />

for the composites in which the ENSO <strong>and</strong> the PDO are in the same (opposite)<br />

phase for austral summer <strong>and</strong> autumn seasons. So, the WPDO (CPDO) background<br />

modulates the ENSO-effects in SSA rainfall, enhancing EN (LN) <strong>and</strong> weakening<br />

LN (EN), during austral summer <strong>and</strong> autumn months. The connection of the PDO<br />

phases <strong>and</strong> ENSO-related rainfall anomalies in SSA is similar to the PDO modulations<br />

of ENSO signals in the rainfall in the Northwest/southwest United States analyzed<br />

by Gershunov <strong>and</strong> Barnett (1998). The differences of EN-related rainfall<br />

composites in SSA between the WPDO <strong>and</strong> CPDO regimes might be explained<br />

comparing the corresponding SST composites. The SST composites for the WPDO<br />

(CPDO) regime resemble the SST anomaly pattern associated with EN conditions<br />

in the equatorial eastern Pacific <strong>and</strong> cold (warm) conditions in the subtropical<br />

south-central Pacific defined by Barros <strong>and</strong> Silvestri (2002) <strong>and</strong> Vera et al. (2004).<br />

So, a possible explanation for the differences in EN rainfall composites in SSA for<br />

the WPDO <strong>and</strong> the CPDO phases lies in the circulation anomalies characterizing<br />

differences in EN response in the South Pacific as shown by Vera et al. (2004).<br />

Another important aspect shown in the present analysis consists of the nonlinear<br />

components of the composites relative to the ENSO phases for a given PDO<br />

phase. It is worthwhile mentioning that the ENSO-related precipitation anomaly<br />

patterns with positive (negative) values in SSA for EN (LN) events documented in<br />

previous studies (Walker 1928; Caviedes 1973; Hastenrath <strong>and</strong> Heller 1977;<br />

Kousky et al. 1984; Ropelewski <strong>and</strong> Halpert 1987, 1989; Aceituno 1988; Kayano<br />

et al. 1988; Kiladis <strong>and</strong> Diaz 1989; Kayano 2003; Grimm 2003) represent in fact<br />

the linear component of ENSO-effects in SSA rainfall. In order to take into account<br />

the non-linear component of the ENSO-effects in SSA rainfall, EN <strong>and</strong> LN composites<br />

should be considered separately. The sequences of monthly rainfall of the<br />

ENSO composites for SSA rainfall in figures 14.1 to 14.4 might provide guidance<br />

for future climate monitoring <strong>and</strong> forecasting purposes for this region.<br />

Another aspect that should be also taken into account for these purposes is the<br />

phase of the PDO. Concerning to this, several studies have suggested that the PDO<br />

shifted back into the cold regime in the late 1990 (Hare <strong>and</strong> Mantua 2000; Schwing<br />

<strong>and</strong> Moore 2000; L<strong>and</strong>scheidt 2001). If the PDO is now in a cold regime, EN-related<br />

<strong>and</strong> LN-related composites for the CPDO phase (Figs. 14.2 <strong>and</strong> 14.4) are more<br />

appropriate guides to estimate future hydro-meteorological conditions in SSA,<br />

while the cold regime lasts.<br />

The authors were partially supported by the Conselho Nacional de<br />

Desenvolvimento Científico <strong>and</strong> Tecnológico of Brazil. Thanks are due to the UK<br />

Meteorological Office (UKMO) for the provision of the sea level pressure data used<br />

in this paper. Thanks are also due to Dr. Mike Hulme for the provision of the<br />

´gu23wld0098.dat´ (version 1.0) constructed at the Climatic Research Unit,<br />

University of East Anglia, Norwich, UK.<br />

196

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