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Chapter 15 Moisture
15-1 Changes of state:
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Common states: Solid, liquid, and gas
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Where is the heat? Heat stored, called latent heat.
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Melting point: the temperature at which solid changes into
liquid.
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Boiling point: the temperature at which liquid changes into
gas.
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To maintain T constant at M. P. and B. P., heat is wither
absorbed from the environment or released to the environment.
15-2 Humidity:
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Vapor pressure: water has vapor, vapor contribute to
pressure. When equilibrated at a particular T, if water evaporation =
water condensation ==> saturation of water vapor in air. It is T
dependent. As T increases, saturation increases.
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Humidity: describe the amount of water vapor per amount
of air.
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Specific humidity:
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Relative humidity (R. H.): water vapor content of air
divided by maximum water vapor content of the air, e.g. at 85 F, max
water vapor content = 26.5 g. If air has 13.3 g of water, the relative
humidity = 13.5/ 26.5 = 0.5 = 50 %.
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Changes in R. H.: R. H. is a function of T. As the T
increases, R. H. decreases. E. g. at 68 F, maximum water vapor content =
14 g. If the air has 13.5 g of water vapor, the relative humidity =
13.5/14 = 100 %.
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Dew point: the T at which R. H. = 100 %.
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Measurement: one type: use the hair length. Longer when
R. H. is high. The other type: use evaporation of water to cool a
thermometer.
15-3 Clouds:
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Adiabatic temperature change:
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When air compressed, T increases, and when air expanded,
T decreases. The former can be felt by pumping a bicycle and the latter
by release of a balloon.
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For unsaturated air: when air goes up, P decreases,
thus, air expand, thus T decreases. Therefore, T decreases by 10 degrees
per 1000 m.
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For saturated air: air is already at dew point, heat due
to condensation is released, which offset the soling rate. Therefore, T
decreases 5 degrees per 1000 m.
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Cloud formation:
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Stable air vs. unstable air:
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Environmental lapse rate: T decreases in the troposphere
~ 6.5°C/1000
m. Varies. Dry adiabatic rate is: ~ 10°C/1000
m, while wet adiabatic rate is: ~ 5°C/1000
m. Fig 15.9. So, as the air heated up, it rises. As it rises, it
cools adiabatically.
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Stable Fig. 15.11: Dry air. Air at 25°C
at the surface. At 1000 m, outside the cloud, the T is 20°C,
due to environmental lapse rate. But inside the cloud, it is 15°C,
due to dry air rate. Thus, it has tendency to sink. Therefore, air
doesn't rise infinitely ==> Stable.
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Absolute stability: Environmental lapse rate < wet
adiabatic rate, e.g. Fig. 15.12. Thus, as air rise the difference
between T inside and outside a cloud gets bigger.
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Temperature inversion: Atop warm air above a cool air,
e.g. Fig. 15B. Warm air behave as a cover to prevent air rise
further.
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Absolute instability: Environmental lapse rate > dry
air rate. Fig. 15.13, in this case, air keeps rising.
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Conditional instability: Wet adiabatic rate <
environmental lapse rate < dry adiabatic rate. In this case, the
cloud is stable when air is not saturated, but not stable when air is
saturated. Fig. 15.14.
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Summary: stable: resist vertical movement. Unstable:
rise vertically.
15-4 Air lifting process:
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Orographic lifting: Mountains behaves as a barrier, air
lift when meet with the mountain. Fig. 15.16. Typical, e.g. Mt.
Olympic. Consequences: windward: wet, precipitation on mountain;
leeward: dry, desert.
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Frontal wedging: when warm air meets with cool air, warm
air wedge up, often associated with precipitation. Fig. 15.18.
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Convergence: Two air masses flow toward each other,
resulting lift, e.g. Florida.
15-5 Air Cloud formation:
To form cloud, fog, or dew, saturation reaches first.
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Two ways to cause saturation: (a) when air temperature
decreases; (b) when more water vapor introduced.
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Supersaturation vs. condensation: When relative humidity
~ 100 %, water vapor reaches saturation, but to form condensation (like
dew drops) nuclei needed. Otherwise, the relative humidity > 100% is
needed to cause condensation.
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Types of nuclei: microparticles and dusts. They are
hydroscopic (means like water). Initial droplets are tiny, gravitational
pulling is negligible.
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Cloud: consists of water droplets, ice crystals (if T
< 0°C),
or both.
15-6 Types of clouds:
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Based on forms and heights.
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High cloud: associated with cirro.
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T low, moisture low.
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thin and white.
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not precipitation maker.
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Middle cloud: alto as prefix.
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Low cloud:
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thicker and gray.
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associated with precipitation.
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nimbostratus: cloud causing large area rain.
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cumulonimbus: cloud causing T-storm.
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Nimbus: rain.
15-7 Fog:
A type of special cloud whose base is near the surface.
Types of fog:
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Advection fog: warm, moist air over cool surface, e.g. fog
in Oregon. Warm air from Pacific over cold current ==> fog ==> wind
carried to land.
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Radiation fog: occurs at night. T decreases due to
radiation, dissipation of heat, air cool, and reach due point. Form fog
pockets in low area.
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Due to addition of moisture: over lake in Fall, water warm,
produced warm air, meeting cold air and fog forms below cold air.
15-8 Precipitation:
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Bergeron Process: due to supercooling and supersaturation.T
of water is below 0°C.
Why not ice? due to lack of nuclei for crystallization. Under this
condition, the relative humidity is > 100 % with respect to ice. Thus,
ice grows bigger and consume more water from vapor. Fig. 15.24.
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Results: ice crystals get bigger and water droplets get
smaller. As crystal size grow big, free fall starts to form
precipitation. If the T > 0°C,
form rain, otherwise, snow.
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Collision-coalescence process: large droplets coalescence
smaller droplets for form even larger one. If too large, > 5 mm, they
break. Fig. 15.25.
15-9 Types of precipitation:
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Rain drizzle: depending on rain drop size. Rain > 0.5 mm.
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Snow: ice crystals. As T decreases, moisture decreases, not
enough water to crystallize ==> fluff snow.
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Sleet: T at upper layer is > 0°C.
Thus, water droplets form. But bottom layer cold ==> sleet forms.
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Hail: upward movement of cloud faster to hold large
particles against the gravitational force.
Homework:
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Read chapter summary on p.436.
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Use your own word to explain the key terms on page 437.
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Answer the review questions on page 437.
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