NATS 101 Section 13: Lecture 20 Atmosphere-Ocean Interactions.
NATS 101 Lecture 2 Vertical Structure of the Atmosphere.
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Transcript of NATS 101 Lecture 2 Vertical Structure of the Atmosphere.
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NATS 101
Lecture 2
Vertical Structure of the Atmosphere
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Vertical Structure of the atmosphere
1. Pressure
2. Density
3. Temperature
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30
Height(km)
20
10
0
Can be thought of as weight of air above you.
(Note that pressure acts in all directions!)
So as elevation increases, pressure decreases.
Higher elevation Less air aboveLower pressure
Lower elevation More air aboveHigher pressure
Pressure:
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Pressure Decreases Exponentially with Height
Logarithmic Decrease
• For each 16 km increase in altitude, pressure drops by factor of 10.
48 km - 1 mb 32 km - 10 mb
16 km - 100 mb 0 km
- 1000 mb
100 mb
10 mb
1 mb
16 km
32 km
48 km
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Equation for Pressure Variation
We can Quantify Pressure Change with Height
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What is Pressure at 2.8 km?(Summit of Mt. Lemmon)
Use Equation for Pressure Change:
p(at elevation Z in km) = pMSL x 10 -Z/(16 km)
Set Z = 2.8 km, pMSL = 1013 mb
p(2.8 km) = (1013 mb) x 10 –(2.8 km)/(16 km)
p(2.8 km) = (1013 mb) x 10 –(0.175)
p(2.8 km) = (1013 mb) x 0.668 = 677 mb
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What is Pressure at Tucson?
Let’s get cocky…
How about Denver? Z=1,600 m
How about Mt. Everest? Z=8,700 m
You try these examples at home for practice
Use Equation for Pressure Change:
p(at elevation Z in km) = pMSL x 10 -Z/(16 km)
Set Z = 800 m, pMSL = 1013 mb
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______Density: = (kg/m3 or g/cm3)
massvolume
Initial State
Incompressible fluid
Initial State
Compressible fluid
The density of the gases that make up the atmosphere is constantly changing. In addition, the atmosphere is compressible.
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Sea-level
Near sea level, air density ~ 1.2 kg m-3.
Denver, CO
At Denver CO, (~1.6 km altitude – or 1 mile), air density is approximately 85% of that at sea level, or 1.01 kg m–3.
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Density and Pressure Variation
Key Points:
1. Both decrease rapidly with height
2. Air is compressible, i.e. its density varies
Ahrens, Fig. 1.5
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“Standard atmosphere” is calculated based on profiles at 30 latitude.
Temperature Stratification
Divide into several vertical layers based on electrical, temperature, and chemical (homogeneous/heterogeneous), characteristics.
Together with the change in density with height, this gives the atmosphere its structure.
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Troposphere
Majority of the weather occurs
here
The lapse rate is theaverage decrease in temperature withheight ~ 6.5°C/km
Contains 80% of the atmospheric
massTropopause
Depth ranges from ~8 km at the poles to ~16 km in
the tropics
Rapid decrease in temperature with
height
Layer of most interest to this course!!!
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Little weather occurs here
Isothermal inlowest 10 km
Lapse rate is 0
Contains ~19.9% of the atmospheric
mass
Stratopause
Temperature increases withheight from 20-~50 km
(Temperature inversion)
Ozone layer
The ozone layer absorbsmuch of the incoming
solar radiation, warmingthe stratosphere, and
protecting us from harmfulUV radiation
Layer of some interest to this course!!!
Stratosphere
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Temperature onceagain decreases
with height
Mesosphere
Temperature onceagain increases
with height
Thermosphere
Neither of these layers have much interest for the Meteorologist
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Ionosphere
- extends from the upper mesosphere into the thermosphere.
Contains large numbers of charged particles called ions. Ions are atoms or molecules that have gained an electron or lost an electron so that they carry a charge. This occurs in the upper atmosphere because the molecules are being constantly bombarded by solar radiation.
Important for reflecting AM radio waves back to Earth.
Also responsible for the aurora borealis (northern lights) and aurora australis (southern lights).
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Divide the atmosphere into several vertical layers based on temperature characteristics. Together with the change in density with height, this gives the atmosphere its structure.
Troposphere
Stratosphere
Mesosphere
Thermosphere
Summary:
Temperature Inversion
Stable layer
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Temperature inversion
tropopause
T-profile
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