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LONGITUDE
LONGITUDE
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(b)
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LONGITUDE
LONGITUDE
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Figure 3.3 Long-term (1984-97) average global distribution of net downward (or absorbed) shortwave radiation (W m -2 ) at the
Earth's surface for the mid-seasonal months of (a) January, (b) April, (c) July and (d) October.
Source: After Hatzianastassiou et al. (2005)
at the surface). When reflected, the radiation is returned
to space in the short-wave form and becomes part of
the outflow of energy from Earth. Similarly, some of the
scattered radiation is returned to space to give a short-
wave albedo for our planet of 28 per cent. The modifica-
tions of the solar beam by the atmosphere are shown
diagrammatically on the left-hand side of Figure 3.2 .
will take place. Clouds are also very effective at absorbing
long-wave radiation and hence their temperature will be
higher than otherwise. This cloud effect is most noticeable
at night. With clear skies and dry air, long-wave radiation
0HDQ
Long-wave radiation
All substances emit long-wave radiation in proportion to
their absolute temperature. Earth's surface absorbs most
short-wave radiation and therefore normally has a higher
temperature than the atmosphere. It follows that more
long-wave emission will be from the ground surface. The
atmosphere is much more absorbent of long-wave
radiation than of short-wave radiation. Carbon dioxide
and water vapour are very effective absorbers of much of
the longer part of the spectrum except between 8 μm and
12 μm. As water vapour is concentrated in the lowest
layers of the atmosphere, that is where most absorption
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Figure 3.4 Average area of the Antarctic ozone hole (mea-
suring <220 Dobson units of ozone) for the period 1996-2005.
Source: Climate Prediction Centre, NOAA, 2006
 
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