chapter - Atmospheric and Oceanic Science
chapter - Atmospheric and Oceanic Science
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 />
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