8) The first table is for the parcel as it travels up the
mountain on the west side.
Altitude (km)
Parcel Temp. Parcel Dew Point.
0
30 C
20 C
1
20 C
20 C <<<< LCL
2
14 C
14 C
3
8 C
8 C - now at the top of the mountain
This next table is for the parcel as
it travels down the east side of the mountain
Altitude (km)
Parcel Temp. Parcel Dew Point.
3
8 C
8 C -- the parcel is saturated AND there are liquid
droplets (a cloud) which provide a source
2
14 C
14 C of water vapor via
evaporation as the parcel travels down the mountain and warms up.
1
20 C
20 C <-Now all the cloud drops have evaporated
since the dew point of the parcel is equal to
0
30 C
20 C the original value (what
we started with journey with). So from here on the rate of warming
would be the dry rate (10 C/km).
The end result is that the air on the east side of the mountain has
the same temperature and dew point as the air on the west side of the mountain.
9) Now whenever condensation occurs, the liquid water is
lost from the parcel via precipitation.
The first table is for the parcel
as it travels up the mountain on the west side.
Altitude (km)
Parcel Temp. Parcel Dew Point.
0
30 C
20 C
1
20 C
20 C <<<< LCL
2
14 C
14 C
3
8 C
8 C - now at the top of the mountain
This next table is for the parcel as
it travels down the east side of the mountain
Altitude (km)
Parcel Temp. Parcel Dew Point.
3
8 C
8 C --- since there is no source of water for evaporation, the warming
rate will be the dry
2
18 C
8 C rate of 10 C/km, and the dew point
will not change.
1
28 C
8 C
0
38 C
8 C
In this case the air on the east side is warmer and drier than the
air on the west side since condensed water left the parcel via precipitation.
As a matter of fact, the air at 0 km on the west side had a relative humidity
of (14g/kg)/(26.g/kg)*100% = 53%, while the air on the east side at 0 km
has a relative humidity of (6.2g/kg)/(42.2g/kg)*100% = 15 %.
As mentioned earlier, the real atmosphere is somewhere in between the
cases a) and b).
a) condensation - drops are first formed via condensation and also during the ice-crystal process
b) ice-crystal process - since the saturation mixing ratio over ice is lower than over liquid water, water will tend to evaporate from the liquid droplets and condense upon ice crystals. The number of ice-crystals is less than the number of liquid droplets, so this process tends to move the water from many liquid drops to a few ice-crystals and thus concentrate the water into relatively big ice-crystals.
c) accretion - this specifically refers to ice-crystals freezing super cooled water droplets when coming in contact with them as the two fall through the atmosphere.