260 Applications and Investigations in Earth Science Because air pressure drops rapidly with increasing altitude above Earth's surface, rising air passes through regions ot successively lower pressure. Therefore, ascending air expands and cools adiabatically. Rising unsaturated air cools at the constant rate of 10°C per 1000 meters (1°C per 100 m). called the dry adiabatic rate. The dry adiabatic rate also applies to descending air, which is compressed and warmed. Once rising air reaches the dew-point temperature and water vapor condenses to form cloud droplets, latent heat that was stored in the water vapor is liberated. The heat released during condensation slows the rate of cooling of the air. Rising saturated air continues to cool by expansion, but at a lesser rate of about 5°C per 1000 meters (0.5°C per 100 m)-the wet adiabaticC rate. Figure 15.9 summarizes this cloud-forming process. Take a minute to carefully examine this figure before beginning Activity 15.8. Height (u) -8°C 000s Wet adiabatic rate (temperature of rising air drops at 5"C/1000 meters) 000 Condensation Y level 0008 12°C Dry adiabatic rate (temperature of rising air drops at 0007 000L Figure 15.9 Adiabatic cooling and cloud formation. Rising air cools at the dry adiabatic rate of 10°C per 1000 meters, until the air reaches the dew-point temperature and condensation (cloud formation) begins. As air continues to rise, the latent heat released by condensation reduces the rate of cooling. The wet adiabatic rate is therefore always less than the dry adiabatic rate. (siajau 0001/0.0 32 C ACTIVITY 15.8 Adiabatic Processes and Cloud Formation Figure 15.10 shows air that begins with a temperature of 25°C and a relative humidity of 50 percent flowing from the ocean over a coastal mountain range. Assume that the dew-point temperature remains constant in dry air (relative humidity less than 100 percent). When the air parcel becomes saturated, the temperature and dew-point temperature become equal. As the air continues to ascend, the temperature and dew-point temperature will decrease at the wet adiabatic rate, but the dew-point temperature does not change as the air parcel descends. (Completing Figure 15.10 may be helpful.) 1. Use Table 15,2 to determine the saturation mixing ratio, water-vapor content, and dew-point temperature of the air at sea level in Figure 15.10. Saturation mixing ratio: g/kg of air 01 Water-vapor content: g/kg of air Dew-point temperature: °C CI 2. Is the air at sea level saturated or unsaturated? unsaturated w 0008 Temp. Dew pt. Dew pt. 2000m Temp. Dew pt. Temp. F. Dew pt. w 0001 Temp. Temp. Dew pt. Temp, at Point A = 25°C Relative humidity at Point A = 50% Dry adiabatic rate = 10°C/1000 meters Wet adiabatic rate = 5°C/1000 meters Dew pt. Sea level A Figure 15.10 Adiabatic processes and cloud formation associated with air being lifted over a mountain barrier.

Applications and Investigations in Earth Science (9th Edition)
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ISBN:9780134746241
Author:Edward J. Tarbuck, Frederick K. Lutgens, Dennis G. Tasa
Publisher:Edward J. Tarbuck, Frederick K. Lutgens, Dennis G. Tasa
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Fill in the values for Figure 15.10.

260 Applications and Investigations in Earth Science
Because air pressure drops rapidly with increasing altitude
above Earth's surface, rising air passes through regions of
successively lower pressure. Therefore, ascending air expands
and cools adiabatically. Rising unsaturated air cools at the
constant rate of 10°C per 1000 meters (1°C per 100 m),
called the dry adiabatic rate. The dry adiabatic rate also
applies to descending air, which is compressed and warmed.
Once rising air reaches the dew-point temperature and
water vapor condenses to form cloud droplets, latent heat
that was stored in the water vapor is liberated. The heat
released during condensation slows the rate of cooling of
the air. Rising saturated air continues to cool by expansion,
but at a lesser rate of about 5°C per 1000 meters (0.5°C per
100 m)-the wet adiabatic rate. Figure 15.9 summarizes this
cloud-forming process. Take a minute to carefully examine
this figure before beginning Activity 15.8.
Height
(u)
-8°C
Wet
adiabatic rate
000S
(temperature of
rising air drops at
5°C/1000 meters)
-3°C
000
Condensation
2°C
000
level
12°C
Dry
adiabatic rate
000
(temperature of
rising air drops at
10°C/1000 meters)
22°C
000
Figure 15.9 Adiabatic cooling and cloud formation. Rising
air cools at the dry adiabatic rate of 10°C per 1000 meters, until
the air reaches the dew-point temperature and condensation
(cloud formation) begins. As air continues to rise, the latent heat
released by condensation reduces the rate of cooling. The wet
adiabatic rate is therefore always less than the dry adiabatic rate.
32°C
ACTIVITY 15.8
Adiabatic Processes and Cloud Formation
Figure 15.10 shows air that begins with a temperature of 25°C and a relative humidity of 50 percent flowing from the
ocean over a coastal mountain range. Assume that the dew-point temperature remains constant in dry air (relative humidity
less than 100 percent). When the air parcel becomes saturated, the temperature and dew-point temperature become
equal. As the air continues to ascend, the temperature and dew-point temperature will decrease at the wet adiabatic rate,
but the dew-point temperature does not change as the air parcel descends. (Completing Figure 15.10 may be helpful.)
1. Use Table 15.2 to determine the saturation mixing ratio, water-vapor content, and dew-point temperature of the
air at sea level in Figure 15.10.
Saturation mixing ratio:
g/kg of air
01
Water-vapor content:
g/kg of air
Dew-point temperature:
2. Is the air at sea level saturated or unsaturated?
unsaturated
D.
W 000
Temp.
Dew pt.
Temp.
Dew pt.
C.
E.
Temp.
Dew pt.
Temp.
F. Dew pt.
B.
Temp.
Dew pt.
Temp.
Dew pt.
Temp. at Point A = 25°C
Relative humidity at Point A = 50%
Dry adiabatic rate = 10°C/1000 meters
Wet adiabatic rate = 5°C/1000 meters
A.
Sea level
A Figure 15.10 Adiabatic processes and cloud formation associated with air being lifted over a
mountain barrier.
Transcribed Image Text:260 Applications and Investigations in Earth Science Because air pressure drops rapidly with increasing altitude above Earth's surface, rising air passes through regions of successively lower pressure. Therefore, ascending air expands and cools adiabatically. Rising unsaturated air cools at the constant rate of 10°C per 1000 meters (1°C per 100 m), called the dry adiabatic rate. The dry adiabatic rate also applies to descending air, which is compressed and warmed. Once rising air reaches the dew-point temperature and water vapor condenses to form cloud droplets, latent heat that was stored in the water vapor is liberated. The heat released during condensation slows the rate of cooling of the air. Rising saturated air continues to cool by expansion, but at a lesser rate of about 5°C per 1000 meters (0.5°C per 100 m)-the wet adiabatic rate. Figure 15.9 summarizes this cloud-forming process. Take a minute to carefully examine this figure before beginning Activity 15.8. Height (u) -8°C Wet adiabatic rate 000S (temperature of rising air drops at 5°C/1000 meters) -3°C 000 Condensation 2°C 000 level 12°C Dry adiabatic rate 000 (temperature of rising air drops at 10°C/1000 meters) 22°C 000 Figure 15.9 Adiabatic cooling and cloud formation. Rising air cools at the dry adiabatic rate of 10°C per 1000 meters, until the air reaches the dew-point temperature and condensation (cloud formation) begins. As air continues to rise, the latent heat released by condensation reduces the rate of cooling. The wet adiabatic rate is therefore always less than the dry adiabatic rate. 32°C ACTIVITY 15.8 Adiabatic Processes and Cloud Formation Figure 15.10 shows air that begins with a temperature of 25°C and a relative humidity of 50 percent flowing from the ocean over a coastal mountain range. Assume that the dew-point temperature remains constant in dry air (relative humidity less than 100 percent). When the air parcel becomes saturated, the temperature and dew-point temperature become equal. As the air continues to ascend, the temperature and dew-point temperature will decrease at the wet adiabatic rate, but the dew-point temperature does not change as the air parcel descends. (Completing Figure 15.10 may be helpful.) 1. Use Table 15.2 to determine the saturation mixing ratio, water-vapor content, and dew-point temperature of the air at sea level in Figure 15.10. Saturation mixing ratio: g/kg of air 01 Water-vapor content: g/kg of air Dew-point temperature: 2. Is the air at sea level saturated or unsaturated? unsaturated D. W 000 Temp. Dew pt. Temp. Dew pt. C. E. Temp. Dew pt. Temp. F. Dew pt. B. Temp. Dew pt. Temp. Dew pt. Temp. at Point A = 25°C Relative humidity at Point A = 50% Dry adiabatic rate = 10°C/1000 meters Wet adiabatic rate = 5°C/1000 meters A. Sea level A Figure 15.10 Adiabatic processes and cloud formation associated with air being lifted over a mountain barrier.
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