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Atmospheric Research
In this chapter we start
with the atmosphere, since the sunlight arriving at the
planet's surface is influenced by it, and thus climate
and winds. The main current systems
in the oceans arise from winds blowing over the water's
surface. See also wind and waves Where such winds blow
for prolonged periods and with sufficient force, the
ocean's water will be moved at speeds between 0.5 and 2
km/hr, contributing directly to the heat transport
towards the poles. Much of the climate depends on these
currents, which in tur n , depend on the climate. Both
the weather and the ocean currents are therefore in
constant oscillation or instability. One of these is the
El Nino climate/current cycle that influences rainfall
and drought far afield and which will be treated in
detail in its own chapter. Also ocean productivity
depends largely on upwellings caused by ocean currents.
More of that in the chapter on plankton and how to feed
the world. Ultimately, the health and physics of the
oceans, plays an important role in the way our pl anet
will warm in response to the burning of fossil fuels.
That too, will have its own chapter.Because the
circulation of water and air depend on the amount of
heat arriving at the planet's surface, it is important
to understand what ha ppens to the sunlight from the
moment it enters our atmosphere. This simple picture
helps to relate the relative distances involved. If the
planet were the size of a billiard ball, say 5 cm across,
then the whole surface of the planet, from Mt. Everest
to the deepest ocean trough (20 km) would be no thicker
than a human hair. Here is where everything happens to
life (the biosphere). Within this human hair, there are
at least two layers in the atmosphere and two in the
ocean that move almost independently o f one another.
\line At a distance of 150-300 km, the atmosphere is so
thin that spacecraft can orbit there in low orbit. The
geostationary satellites orbit some 36000 km higher, a
distance of about six times the radius of Earth. The at
mosphere is a blanket of protective gases providing
insulation against otherwise extreme alterations in
temperature. Earth's gravity pulls the gases towards its
surface where the pressure is 1 bar, decreasing rapidly
with height. At 100 km height, the pre s sure is only
one millionth. About 80% of the atmosphere is found in
the first 15 km; half in the first 5 km. In the diagram,
the various zones are shown. Note that their boundaries
vary appreciably from pole to equator and from day to
night. The outer zon e is the exozone which gradually
fades into space. At 600 km the pressure is a mere 1E-38
bar or less than a trillionth of a trillionth of a
trillionth of surface pressure. Only the fastest atoms
of the lightest gases, Hydrogen and Helium are found
here. Close to the surface, the troposphere (between 8
km at the poles and 15 km at the equator) is where the
weather and climate reign. It contains 85% of the
atmospheric mass. Air temperature falls steadily at
about 4-8\'baC for every km height, 8\'baC at the
tropics and almost nil at the North Pole in winter.
Where the passenger airliners fly, 10 km, the
temperature is -60 degrees, varying with day and night
and other conditions. Near the surface of Earth, the
temperature is on average 15 degrees and the air is
composed of 78% nitrogen, 21% oxygen and 1% argon. The
tropopause is a region where the temperature starts to
rise again, forming the boundary with the stratosphere,
which extends upward to 50 km. Here is where protective
ozone is found (20-50 km). The stratosphere absorbs
ultraviolet light, which warms it. Just above the ozone
layer, the temperature drops again gradually to -80
degrees at the mesopause. In the ionosphere, air
particles are electrically charged by the sun's
radiation, being able to move at high speeds in the
almost perfect vacuum. The temperatures shown in the
diagram, therefore have little meaning. A space craft in
this zone would not experience it. Four electrically
charged layers are found here, the D, E, F1 and F2
layers. These are c a pable of bouncing radio waves of
various frequencies, enabling radio transmitters to beam
their programmes much further. Short-wave radio
frequencies are able to reach the other side of the
planet under favourable conditions. Medium wave (MW)
transmission s benefit from the D layer, which becomes
active in the night. Polar auroras occur between 65 and
965 km height in the polar regions. Meteors from outer
space burn up in the lower ionosphere, at around 100-150
km height.
Atmospheric Gravity waves
Gravity waves are the oscillations of air parcels by
the lifting force of bouyancy and the restoring force of
gravity. These waves propagate vertically as well as
horizontally, and actively transport energy and momentum
from the troposphere to the middle and upper atmosphere.
Gravity waves are caused by a variety of sources,
including the passage of wind across terrestrial
landforms, interaction at the velocity shear of the
polar jet stream and radiation incident from space. They
are found to affect atmospheric tides in the middle
atmosphere and terrestrial weather in the lower
atmosphere. Gravity waves are investigated using
pressure sensors, in situ aircraft measurement, and
imaging data. Gravity waves are often seen in the lower
atmosphere (~10 km) by thin bands of cloud and sky.
Higher in the atmosphere (80-100km), gravity waves can
be 'seen' in moving bands of atmospheric air glow. The
airglow emits spectra from chemiluminescence of
atmospheric molecules. By analyzing the motion of
different spectramesospheric gravity waves can be
roughly plotted.
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