The growth of geographically confined errors is studied in six experim
ents with a five-level global spectral (rhomboidal 30) general circula
tion model. Each experiment consists of 36 identical twin integrations
with the initial errors localized in the same region. The centers of
the regions are 180-degrees, 120-degrees-W, 60-degrees-W, 0-degrees, 6
0-degrees-E, and 120-degrees-E; all at 45-degrees-N. The perturbations
are derived from differences in model states taken from a long integr
ation. They reflect the natural distribution of variance in the model
atmosphere, and are representative of realistic analysis errors.By day
10 the errors have propagated (predominantly eastward) until they hav
e reached either of the oceanic baroclinic waveguides and have amplifi
ed dramatically there. Errors originating in the central Pacific or we
stern North America amplify over the Atlantic. Errors from the Europea
n, central Asian, and East Asian regions grow most strongly over the P
acific. Errors originating over the Atlantic show a mixed behavior. Th
e rates of propagation involved are consistent with the downstream dev
elopment of baroclinic instability. The behavior of the errors normali
zed by the climatological variance is similar. The cause of preferenti
al error growth in the oceanic waveguides is the markedly baroclinic s
tructure of the errors in these regions. The largest 10-day errors ori
ginate in the Pacific and grow and propagate into the Atlantic, while
the smallest ten-day forecast errors arise from initial errors over Eu
rope. The largest 10-day relative error (error divided by its initial
value) arise from errors originally confined to East Asia and Asia, wh
ich develop over the Pacific. The experiments with perturbations cente
red at 60-degrees-E, 120-degrees-E, and 180-degrees were repeated usin
g initial errors that were identical in structure and magnitude but we
re zonally translated. At day 10 the errors that originate over the Ea
st Asian coast and developed in the mid-Pacific were the largest. The
relative error in these modified experiments behaved very much like th
at in the original experiments. After the initial period of growth, a
stagnation of the errors is seen in the primary of the two oceanic are
as, accompanied by error growth in the other (secondary) oceanic regio
n. For certain experiments (those with initial errors in the Pacific,
Asia, and East Asia) the latter development can be quite rapid. There
is a substantial variation in the growth rates from case to case, with
the rms of the most rapidly growing perturbation as large as three ti
mes that of the average. The identity of the pair of states leading to
the largest error depends on the forecast time.