| How Clouds Form |
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Clouds form when the air cools to the dewpoint (the temperature
at which air becomes saturated and the previously invisible
water vapour condenses into tiny droplets).
Cooling occurs in two basic ways:
- air either comes into contact with a cold surface (the
will occur when moist air passes over cold land or sea to
give low stratus cloud)
or rises in the atmosphere (air may rise when there is convection
caused by heating, it is forced over hills or mountains
or if it encounters colder, denser air).
- Another process, convergence, occurs when air is forced
into a restricted area. Some of the air must rise to escape.
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| Stability |
Darren Dowling
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Warm air rises, expands and cools. How far it moves depends
on the surrounding air. If this is relatively warm it has
a lower lapse rate, so the rising air cools faster than its
surroundings. When it reaches the same temp. as its surroundings
it stops. Such conditions are said to be stable and lead to
the formation of stratiform clouds if the rising air does
not reach the dewpoint.
If however the surrounding air is relatively cold a rising
parcel of air may remain surrounded by colder air and continue
to rise. The conditions are unstable and result in cumuliform
clouds. The rising air may even accelerate, especially if
it reaches the dewpoint and condensation occurs.
Instability (and cumulus clouds) are often found in cold
air flowing over a warm sea. Warm air moving over cold land,
by contrast, is stable and frequently produces low stratus
cloud. An inversion is a layer where temperature increases
with height, so inversions are layers of extreme stability.
They often cause the upward growth of clouds to come to a
halt.
Stratocumulus and altocumulus often arise when cumulus clouds
encounter and inversion.
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| Inversions |
Darren Dowling
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Temperature tends to decrease with height (at least in
the lower reaches of the atmosphere). The rate at which the
temperature falls (called the lapse rate) averages about 6
°C per km. However this rate is not constant (as the air
consist of various layers of different temperatures and humidities).
In certain layers, known as inversions, temperature actually
increases with height.
A major inversion, called the tropopause, defines the boundary
between the troposphere and the overlying stratosphere. Above
the tropopause, temperature increases rapidly throughout the
stratosphere, up to about 50 km (mainly because ozone absorbs
a great deal of UV radiation from the Sun).
The tropopause height depends on latitude and season but
is at about 16-18 km over the equator, 11-12 km at middle
latitudes and around 8-9 km over the poles.
The tropopause limits the growth of the most vigorous cumulonimbus
clouds, and forces them to expand sideways into large cirrus
anvils (it is not a complete barrier though).
Air conducts heat poorly. Once away from the surface a parcel
of air cools or warms almost independently of it surroundings.
The rate at which rising air cools depends on the amount of
water vapour present. All air contains water vapour but when
it is above its dewpoint no water droplets are present and
it is described as 'dry'. Dry air cools at around 10 °C
per km.
Because heat is needed to evaporate water the reverse process,
condensation, releases this latent heat. Once air has cooled
to the dewpoint, cloud droplets form and the heat released
reduces the rate of cooling. As a result, saturated air cools
at a lower rate, about 5 °C per km.
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| Convection |
Darren Dowling
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Convection is a familiar process and occurs when a gas
or liquid is heated from below. In the atmosphere it is responsible
for most of the pressure differences. Above ground heated
by the Sun or other sources, invisible bubbles of warm air
(thermals) break away from the surface and rise up. The thermals
expand and cool as they rise and eventually reach the dewpoint.
The type of cloud that then forms depends entirely upon the
way in which the temperature of the surrounding air varies
with height and upon whether the air is stable or unstable.
Convection generally produces cumuliform clouds but may produce
stratocumulus and altocumulus.
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| Orographic Clouds |
Darren Dowling
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These are clouds formed by forced uplift over hills or mountains.
The cloud type depends on the stability. Just as air cools
when it rises it also warms at the same rates when it descends.
On the sheltered side of hills and mountains cloud droplets
evaporate and any cloud tends to break up and disperse.
With the right combination of stable conditions, trains of
waves may be set up, bringing air down from upper warmer levels
in the shelter of the mountains. This may be warmer and dryer
than air at the same height on the windward side and this
will cause a dramatic temperature rise accompanied by extremely
dry air and the rapid disappearance of snow (the 'fohn' effect).
When conditions are unstable, cumuliform clouds form.
In the final process of cloud formation, cold air lifts warm
air away from the surface. This occurs at the warm and cold
fronts of depressions.
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