MARCOULIDES MOUSTAKI-Latent Variable and Latent Structure Models
Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616
Transcript of Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616
![Page 1: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/1.jpg)
Physical GeographyChapter 5
Clouds and Precipitation:The Transfer of Latent Heat
![Page 2: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/2.jpg)
The Global Water Budget•Earth has a global water budget—if
water is lost in one place or in one form, it is moved to another place or another form
•The total amount of water (in whatever form) varies from place to place, but stays constant over the planet as a whole
![Page 3: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/3.jpg)
Where is all of Earth’s water found?
•Oceans = 97.2%•Glaciers = 2.0%•Underground sources
(aquifers, underground pools & groundwater) = 0.5%•Lakes (half saline, half fresh) = 0.2%•Pore spaces in soil (“soil water”) = 0.04%•Atmospheric water, streams, living things = 0.01%
![Page 4: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/4.jpg)
The Hydrologic Cycle•The hydrologic cycle is the planetary circulation
of water within and between the different sources of water on Earth—it is a closed system.
•The power source behind the hydrologic cycle is the radiant energy of the sun.
![Page 5: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/5.jpg)
Residence Time•The amount of time a given amount
of water may remain in a particular segment of the hydrologic cycle is its residence time.
•Residence time can vary from hours (evaporation followed by a thundershower), to millions of years (trapped in deep aquifers)
![Page 6: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/6.jpg)
Residence Time•As water changes its “residence,” it may
also change state.•When water changes state it moves
around latent heat. The evaporation and condensation phase changes are especially significant...
How about a diagram???
![Page 7: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/7.jpg)
Latent Heat Transfer
evaporation—latent heat absorbed
condensation—latent heat released
melting—
latent heat absorbed
freezing—latent heat released
ice (solid)
water vapor (gas) water (liquid)
depo
sitio
n—la
tent
hea
t rel
ease
d
subl
imat
ion—
late
nt h
eat a
bsor
bed
![Page 8: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/8.jpg)
Saturation The saturation point is the point at which a given parcel
of air is holding the maximum amount of water vapor that it can possibly hold at a given temperature and pressure.
– Temperature is the key! If the air is not saturated, evaporation can continue, as
long as there is moisture available to be evaporated
![Page 9: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/9.jpg)
Three Factors Influencingthe Rate of Evaporation
1. Temperature of the water– The warmer the water, the faster the
molecules are moving and the more likely they will be able to escape the surface (evaporate)
![Page 10: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/10.jpg)
Three Factors Influencingthe Rate of Evaporation
2. Temperature of the air– Warm air can hold more water vapor
suspended in it– Warm air transfers heat to the water and
speeds up water molecules to the point where they can evaporate
– Cold air can hold less water as a vapor and reaches its saturation point more quickly
![Page 11: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/11.jpg)
Three Factors Influencingthe Rate of Evaporation
3. Degree of windiness– Saturation is reached quickly right above the
water– Wind blowing over a wet surface will reduce
saturation above that surface by moving water vapor molecules away from the surface. This leaves room for more molecules to evaporate
![Page 12: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/12.jpg)
Vapor Pressure
Vapor pressure--the portion of total air pressure made up of water vapor molecules
Saturation vapor pressure--the pressure exerted by the maximum amount of water vapor a parcel of air can hold at a given temperature.
12
![Page 13: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/13.jpg)
![Page 14: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/14.jpg)
Relative Humidity The amount of water vapor in the air at a given temperature,
compared with the maximum amount of water vapor which could be in the air if it were saturated
RH = actual/maximum x 100 = ___ %
RH = relative humidity Actual = the actual amount of water vapor in the air right now Maximum = the maximum amount of water vapor the air can hold at
the given temperature and pressure (in other words, saturation point)
![Page 15: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/15.jpg)
RH Example:
If the room you’re sitting in has 5 grams of water vapor actually suspended in it, but the maximum amount of water vapor that the air could possibly hold is 10 grams, then:
RH = actual/maximum x 100 = ___ %
RH = 5g / 10g x 100 = 50%
![Page 16: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/16.jpg)
Relative Humidity What happens when relative humidity
reaches 100%?– Saturation– Condensation
Clouds or fog (if cooling continues)
![Page 17: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/17.jpg)
Two Ways to ChangeRelative Humidity
Change the temperature of the air– Temperature up, RH down– Temperature down, RH up
Add or subtract water vapor– In the atmosphere, water is added through evaporation,
or lost through precipitation (rain, snow, etc.)
![Page 18: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/18.jpg)
The Dew Point
The dew point is the temperature at which saturation is reached.
![Page 19: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/19.jpg)
The Adiabatic Process
What’s
happening,
here?
![Page 20: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/20.jpg)
The Adiabatic Process
The process by which rising air cools (as it expands) and sinking air warms (as it is compressed) in the atmosphere
The physical principle involved:– When a gas expands, it cools– When a gas is compressed, it warms
![Page 21: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/21.jpg)
The Adiabatic Process As an air mass rises through the atmosphere, it
moves into an area of lower density, allowing the molecules the freedom to expand.
As air expands, there are fewer collisions between molecules and the air begins to cool.
So rising air expands and cools down. If the air mass cools enough to reach the dew point temperature, condensation will occur and a cloud will form.
![Page 22: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/22.jpg)
The Adiabatic Process On the other hand, a sinking air mass will move down
through the atmosphere into a region of increasingly more molecules of air.
The pressure of all of these molecules will compress the air mass, forcing the molecules closer to one another.
This increases the number of molecular collisions, speeding up the molecules, which translates into an increase in temperature.
So sinking air is compressed and warms up.
![Page 23: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/23.jpg)
The DAR
The rate at which unsaturated air will cool as it rises is called the Dry Adiabatic lapse Rate, or DAR (the air is not actually “dry”, it’s just not saturated).
Although this rate can vary based on several atmospheric variables, a commonly-used average value is:
10ºC/1000m (5.5ºF/1000ft)
![Page 24: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/24.jpg)
The LCL
The lifting condensation level (LCL) is the elevation at which condensation occurs.
As it rises, expands, and cools, the air’s relative humidity increases (getting closer to 100%) until eventually the air parcel reaches its dew point temperature.
At that point, saturation has been reached and a cloud begins to form.
The elevation where this happens is the LCL.
![Page 25: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/25.jpg)
You can “see” the LCL:Look at the flat bottom of the cloud
![Page 26: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/26.jpg)
A Quick Reminder!
The following five conditions all occur at the same time:
Saturation Condensation RH=100% Dew point temperature LCL (lifting condensation level)
![Page 27: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/27.jpg)
The Latent Heat of Condensation
Once condensation occurs, the water molecules begin to give off the latent heat of condensation. This heat becomes sensible heat that can be measured.
This heat interferes with the adiabatic cooling that is going on, slowing down the cooling process. So the air continues to get colder as it rises, but it cools at a slower rate.
![Page 28: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/28.jpg)
The SAR (or MAR) The rate at which a saturated parcel of air will
cool as it rises is called the Saturated Adiabatic lapse Rate, or SAR (also called the MAR, or moist adiabatic lapse rate)
Again, the rate varies, but we’ll use an average value of:
5ºC/1000m (3.3ºF/1000ft) As the air parcel continues to rise, it
continues to cool, though more slowly.
![Page 29: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/29.jpg)
Buoyancy– The tendency of a substance to rise, especially in a fluid
An air-filled balloon (or you!) in water A helium balloon in air
– Density is the key Equilibrium level
– Where both the rising and the still air are the same density The opposite of buoyancy is stability
– The substance does NOT want to rise
Stability vs. Buoyancy
![Page 30: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/30.jpg)
Stable air
![Page 31: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/31.jpg)
Unstable air
![Page 32: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/32.jpg)
Conditionally unstable air
![Page 33: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/33.jpg)
![Page 34: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/34.jpg)
Condensation nuclei and cloud droplets
![Page 35: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/35.jpg)
Classifying CloudsAre you paying attention?
![Page 36: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/36.jpg)
Extra Credit Section!!!
![Page 37: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/37.jpg)
Cloud types…
![Page 38: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/38.jpg)
Fog: A cloud on the ground
![Page 39: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/39.jpg)
The Four Common Types of Fog
![Page 40: Physical Geography Lecture 07 - Clouds and Transfer of Latent Heat 102616](https://reader036.fdocuments.us/reader036/viewer/2022062522/58864fff1a28ab32768b70c7/html5/thumbnails/40.jpg)
Dew: Condensation on Earth’s surface