5 Cloud Development Flashcards
Adiabatic Process
•the adiabatic process is important very near earths surface
• moving higher into the atmosphere, the adiabatic process
becomes much more important
• recall that an unsaturated parcel of air cools by 1 °C for every 100 m it
rises – the dry adiabatic lapse rate
• at the same time, the dew point of the air parcel is decreasing, at a rate
of 0.2 °C per100 m – the dew point lapse rate
• the air parcel temperature is approaching the dew point by 0.8 °C
for every 100 m that it rises – eventually the air parcel temperature
reaches the dew point, and saturation is achieved
Level of condensation
the point at which the dry adiabatic lapse rate and dew point lapse rate meet and saturation occurs
-the air parcel then moves at the wet adiabatic lapse rate
Rising to the level of condensation, the dry adiabatic lapse rate is __ degrees/1000m and the dew point lapse rate is __ degrees/1000m
wet adiabatic rate is __degrees/1000m
10
2
5
flat cloud bottoms are cause by the …
level of condensation seperating the dry and wet adiabatic lapse rate
cloud droplets
• saturation is achieved at the lifting condensation level (LCL), and the air
parcel will continue to rise and cool at the saturated adiabatic lapse rate
• condensation onto condensation nuclei begins immediately above the
LCL in the form of small cloud droplets
• as the air continues to rise, small droplets continue to form until all of
the condensation nuclei are consumed – > 50m above the LCL
• since there are no more condensation nuclei, water vapour condenses
onto already existing droplets, making them bigger
• recall the importance of size and curvature, in terms of evaporation
rates
•eventually, the air parcel will stop rising, and condensation will cease
• the adiabatic process is completely reversible
• if the air parcel begins to descend it will do so at the SALR, but evaporation of the cloud droplets will occur
• eventually, the parcel reaches the LCL, evaporation is complete, and
the air parcel continues to sink along the DALR
• if the air parcel reaches the surface again, it will have the same
temperature and dew point as when it started to rise
• this is slightly idealized, since there is a chance that some of the moisture
is lost through precipitation, but this is usually only a minor component
4 types of cloud lifting
- orographic lifting
- frontal lifting
- convergence
- localized convection
orographic lifting
• air flowing across the landscape will be forcibly deflected by
topographic barriers – mountains
• typically, air is forced to rise up and over a mountain range, cooling as it
does so
• condensation occurs and clouds begin to form – orographic clouds
• the height of the clouds is
not restricted by the height
of the barrier –orographic clouds sometimes penetrate into the stratosphere
.this produces the rain shadow effect
• once the air has passed the barrier and begins descending down the
leeward side, it warms adiabatically, and evaporation occurs
•this produces the rain shadow effect – limited cloud cover and little
precipitation occurs on the leeward side of mountains
Frontal Lifting
• cold and warm fronts are generated by the horizontal movement of air and
displacement of the lower density air parcel upward
• in a cold front, colder air pushes into a warmer air mass – the cold air stays near the surface and the warm air is forced to rise • in a warm front, warmer air blows into colder air – the warm air rides up and over the cold, dense air
Convergence
• when air flows into a low pressure centre, it must also be expelled
somehow – the centre cannot hold an infinite amount of air
• the air is forced upwards into the atmosphere
•this is why cyclones are typically accompanied by stormy weather
Localized Convection
- free convection is generated by heating of Earth’s surface
* lifting is generated by the relative buoyancy of warmer air parcels
Atmospheric Cloud Stability
• what happens once lift is initiated?
• this depends on the static stability of the air
• statically unstable air becomes buoyant when lifted and will
continue to rise even after the lifting mechanism has stopped
• statically stable air resists upward movement, and will sink back to its
original position if the lifting mechanism is stopped
• statically neutral air rises by a lifting mechanism, but stops rising
once the mechanism stops – it will not fall back down
•.stability is strongly related to buoyancy
• if the air parcel is warmer than the surrounding air, it has positive
buoyancy and will be statically unstable
• if the air parcel is colder than the surrounding air, it has negative
buoyancy and will be statically stable
Temperature and atmospheric cloud stability
• rates of temperature change are also important
• if a rising air parcel is cooling faster than the air around it, lift will be
suppressed (DALR/SALR > ELR)
• if a rising air parcel is cooling slower than the air around it, lift will
continue (DALR/SALR < ELR)
• the stability of air is therefore dependent on the relative temperature
and density differences between the parcel and the surrounding
environment
the relative density of a rising air parcel depends on:
•.whetehr or not is it saturated
•.the environmental lapse rate
• the relative density of a rising air parcel depends on:
- .whetehr or not is it saturated
* .the environmental lapse rate
Absolute instability of a cloud
.this is known as absolute Instability, and the parcel will continue to rise and t an ever increasing rate
-if the air parcel is saturated it will rise faster and higher because it is even more unstable
If DALR>ELR and Once the lifting mechanisms stops, this air parcel will
sink back down to the ground, this is absolute stability
-the same holds for a saturated air parcel, but in this case the density difference becomes greater in the unsaturated air, so sinking will be faster for unsaturated vs saturated air
conditional instability
• the issue of stability becomes complicated when we recall that the
lapse rate of an air parcel will change once saturation is achieved – the
DALR turns into the SALR
• sometimes, the DALR > ELR but the SALR < ELR
• this is known as conditional instability, and whether or not the air parcel
will rise or sink depends on whether saturation is achieved and how much
lifting has already occurred
level of free convection
marks the altitude to which the air must rise
under force, but above which it will rise due to buoyancy
potential instability
• these examples refer to idealized parcels of air, but what if a large mass
of air was forced to lift off the ground
• in this case, the ELR is forced to change, and is therefore no longer static
• this is called potential instability, and is a particularly important
mechanism for severe storm generation
• this often occurs when warm and dry air sits above warm and wet air
• as these rise, the situation is statically stable, but eventually, they will
rise high enough that the top layer will become colder (and denser)
than the lower layer
• this is because the lower layer will cool slower, at the SALR, than
the top layer which cools quickly at the DALR
• since this is uplift dependent, we can say that the situation is potentially
unstable
Environmental Lapse Rate
its changes due to: 3
• it changes due to:
- heating or cooling of Earth’s surface
- advection of warm and cold air at different levels
- advection of a new air mass
• during the day, insolation warms the surface which warms the lower
atmosphere
• early in the day, the lower troposphere will have a steeper ELR than
higher up, and that steep section will continue to rise as the day
progresses
• at night, cooling of the surface cools the lower troposphere faster producing a night-time inversion