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280
ENSI Erfahrungs- und Forschungsbericht 2011
tween LGM1 and LGM2 are found for the North
Atlantic region especially in winter (December–
January–February, DJF), which is due to the pre-
scribed ocean surface that differs the most in this
area. In LGM2 the winter sea ice extends as far
south as 40°N and the Nordic Seas are widely cov-
ered by ice leading to a strong regional decrease
of SATs compared to PI. In contrast, the less exten-
sive southward sea ice extent in LGM1 leads to a
much less pronounced cooling, so that the two
LGM simulations differ by up to 30 °C over the
ocean especially in the Nordic Seas. As a further
consequence the cooling in Europe downstream
of the strong anomaly is less pronounced in LGM1.
As for the temperature the large-scale annual
mean precipitation anomaly patterns of the LGM
simulations with respect to PI agree well. In the
North Atlantic region the anomaly patterns for
DJF and summer (June–July–August, JJA) share
the main characteristics, namely generally drier
conditions except for a band of increased precip-
itation between 30° to 40°N reaching from the
eastern coast of North America to the Mediterra-
nean in winter and for some tropical region and
parts of the Fennoscandian ice sheet in summer
(Fig. 3a–d). At most locations in the mid- and high-
latitudes the anomalies are larger in winter than
in summer and the differences between LGM1
and LGM2 are more pronounced in winter. Com-
pared to LGM2 the DJF precipitation in LGM1 is
increased in the northern North Atlantic, in the
Nordic Seas, and in parts of the Mediterranean,
while a decrease is found at the lee side of the Fen-
noscandian ice sheet.
The impact of the radiative forcing changes be-
tween the LGM and MW leads to similar differ-
ences as for the ocean surface. The global mean
SAT in MWLGM is 0.8 °C higher than in LGM2,
but slightly lower than in LGM1, and the annual
mean SAT pattern is close to the ones in the LGM
simulations. As the northeastern part of the Atlan-
tic and the Nordic Seas are only partially covered
by sea ice in winter, the strongest anomalies with
respect to LGM2 are located in this region. Gen-
erally, the anomaly pattern is similar to the one
for LGM1, but with reduced amplitude especial-
ly around Newfoundland. Apart from the North
Atlantic the changes correspond to the forcing,
i.e. the southern hemisphere is slightly cooler in
MWLGM due to a strong reduction of solar inso-
lation that overcompensates the increased GHGs
forcing. For JJA, the SATs are globally higher in
MWLGM in agreement with the higher insolation
and the increased GHG concentrations.
The global mean precipitation in MWLGM is of
similar strength as in LGM1 and the spatial distri-
butions of the anomalies with respect to PI resem-
bles the ones of the LGM simulations for the annu-
al mean as well as for DJF and JJA (Fig. 3e and f).
The winter precipitation difference pattern LGM2-
MWLGM is similar to the pattern LGM2-LGM1,
but with reduced amplitudes especially in the sur-
rounding of Newfoundland. In contrast, for sum-
mer precipitation the pattern of LGM2-MWLGM
differs from the one of LGM2-LGM1 showing a re-
Figure 3:
Winter (DJF) and summer
(JJA) precipitation
anomalies with respect
to PI for LGM2 (a and b),
LGM1 (c and d), MWLGM
(e and f), MWLIN (g and
h), and MWUS (i and j).
Only values that are
statistically significant
at the 5 % level based on
the two-sided Student's t
test are colored.
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