If air is forced to rise but has not cooled to its dew point temperature, the air will cool at a constant rate of about 10°C/1000m (5.5°F/1000 ft). This is known as the dry adiabatic rate (DAR). If the rising air cools to its dew point temperature, condensation commences; the air will continue to cool as it rises, but at a rate of about 6°C/1000m (3.2°F/1000 ft). This is known as the moist adiabatic rate (MAR). The MAR is less than the DAR because latent heat is released into the air during condensation. If the air stops its forced ascent, adiabatic cooling will also cease, and there would be no further condensation. If the air were forced to descend (e.g., on the leeward side of a mountain range), the air would heat adiabatically at the dry adiabatic lapse rate of 10°C/1000m. It is important not to confuse adiabatic cooling with the environmental lapse rate (ELR). The environmental lapse rate is simply the decrease in temperature with altitude through stratified air (air that is neither rising or descending) at a particular place and time. For adiabatic cooling or heating to occur, air must be forced to rise or sink, respectively. Summary: DAR = 10°C/1000m 6°C/1000m MAR = ELR varies depending on place and time. In the example below we will use 4.5°C/1000m

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Adiabatic Cooling and Heating.  (See text pp. Section 6.3.)  If a parcel of air is forced to ascend in altitude, it will expand with the lessened air pressure, and it will cool because of the decrease in the number of molecular collisions between air molecules.  Alternatively, if the air parcel is forced to descend in altitude, it will be compressed with the increasing air pressure, and it will warm because of the increased number of molecular collisions.  This is known as adiabatic cooling and heating.  Upon lifting, the air may cool to its dew point.  If so, the air has reached 100% relative humidity and therefore condensation occurs, clouds form, and with sufficient condensation some form of precipitation will result.

If air is forced to rise but has not cooled to its dew point temperature, the air will cool at
a constant rate of about 10°C/1000m (5.5°F/1000 ft). This is known as the dry adiabatic
rate (DAR). If the rising air cools to its dew point temperature, condensation
commences; the air will continue to cool as it rises, but at a rate of about 6°C/1000m
(3.2°F/1000 ft). This is known as the moist adiabatic rate (MAR). The MAR is less than
the DAR because latent heat is released into the air during condensation.
If the air stops its forced ascent, adiabatic cooling will also cease, and there would be no
further condensation. If the air were forced to descend (e.g., on the leeward side of a
mountain range), the air would heat adiabatically at the dry adiabatic lapse rate of
10°C/1000m.
It is important not to confuse adiabatic cooling with the environmental lapse rate (ELR).
The environmental lapse rate is simply the decrease in temperature with altitude
through stratified air (air that is neither rising or descending) at a particular place and
time. For adiabatic cooling or heating to occur, air must be forced to rise or sink,
respectively.
Summary:
DAR = 10°C/1000m
MAR = 6°C/1000m
ELR varies depending on place and time. In the example below we will use 4.5°C/1000m
%3D
Transcribed Image Text:If air is forced to rise but has not cooled to its dew point temperature, the air will cool at a constant rate of about 10°C/1000m (5.5°F/1000 ft). This is known as the dry adiabatic rate (DAR). If the rising air cools to its dew point temperature, condensation commences; the air will continue to cool as it rises, but at a rate of about 6°C/1000m (3.2°F/1000 ft). This is known as the moist adiabatic rate (MAR). The MAR is less than the DAR because latent heat is released into the air during condensation. If the air stops its forced ascent, adiabatic cooling will also cease, and there would be no further condensation. If the air were forced to descend (e.g., on the leeward side of a mountain range), the air would heat adiabatically at the dry adiabatic lapse rate of 10°C/1000m. It is important not to confuse adiabatic cooling with the environmental lapse rate (ELR). The environmental lapse rate is simply the decrease in temperature with altitude through stratified air (air that is neither rising or descending) at a particular place and time. For adiabatic cooling or heating to occur, air must be forced to rise or sink, respectively. Summary: DAR = 10°C/1000m MAR = 6°C/1000m ELR varies depending on place and time. In the example below we will use 4.5°C/1000m %3D
4. Figure 1 illustrates air that is being forced to rise as it crosses over a mountain
range. Assume that as the air rises and cools that it does not cool enough to
reach its dew point. Upon reaching the summit, the air is forced to descend
down the leeward side of the range.
Figure 1
Stratified Air
Rising Air
2300m
1300
300 m
300
a) On Figure 1: Based on the adiabatic rates given on page 2, and assuming an
environmental lapse rate (ELR) of 4.5°C/1000m, calculate and fill in the
temperature (in °C) for the elevations shown for both the rising air, the
nearby stratified air, and for air that has descended on the leeward side of
the mountains
b) Figure 1: How does the temperature of the rising air at the summit compare
with the temperature of the adjacent stratified air at the same elevation?
Why is this so?
c) Figure 1: How does the temperature on the windward side at the base of the
mountain compare with the same elevation on the leeward side? Why is this
so?
Transcribed Image Text:4. Figure 1 illustrates air that is being forced to rise as it crosses over a mountain range. Assume that as the air rises and cools that it does not cool enough to reach its dew point. Upon reaching the summit, the air is forced to descend down the leeward side of the range. Figure 1 Stratified Air Rising Air 2300m 1300 300 m 300 a) On Figure 1: Based on the adiabatic rates given on page 2, and assuming an environmental lapse rate (ELR) of 4.5°C/1000m, calculate and fill in the temperature (in °C) for the elevations shown for both the rising air, the nearby stratified air, and for air that has descended on the leeward side of the mountains b) Figure 1: How does the temperature of the rising air at the summit compare with the temperature of the adjacent stratified air at the same elevation? Why is this so? c) Figure 1: How does the temperature on the windward side at the base of the mountain compare with the same elevation on the leeward side? Why is this so?
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