Atmosphere:
Questions that you should be able to
answer at the end of this lecture:
- How does pressure change with altitude?
- How does temperature change with altitude?
- What are the different layers of the
atmosphere, and how are they identified?
- What is the composition of the atmosphere?
- What are the gases?
- Where did they come from?
- What is the abundance of the gases?
- I will not expect you to know exact
numbers, especially for trace gases, but I do want you to
know approximate values for the 4 most abundant gases.
- You should be able to rank the 4 most
common gases in terms of abundance.
- You should know which gases ARE most
abundant and which are trace gases.
- If they are trending up or down, I want
you to know that.
- What is the importance of the gases?
- What are the pollutants, and why are they
important?
- What is the Greenhouse Effect?
- What causes it?
- Why is it important?
- What is the Radiation Balance?
- What are the numbers?
- What are the components?
- What types of solar radiation are
important?
- What are greenhouse gases?
- Why is the Greenhouse Effect important?
- How does the Radiation Balance control our
temperature?
Link to Weather
Channel
Link
to
US Satellite animation
Average Sea Level Atmospheric Pressure:
14.7 lbs/sq. in. or about 1000 milliBars (mB) [more precisely,
1013mB]
What does this mean?
- On average, over every square inch of the
earth's surface at sea level, there is a force of 14.7
pounds.
- Where does that force come from?
- Imagine a column of air, 1in x 1in (1
square inch), from sea level to the "top" of the
atmosphere (we'll discuss "top" shortly).
- How much would that weigh?
- It would weigh 14.7 lbs.
- The air pressure on the the earth comes
from the mass of the atmosphere over every point, pulled
by gravity; in other words, the weight of the atmosphere
over every square inch of the earth's surface is what
gives us air pressure.
- Given that this is the case, how might you
calculate the weight of the entire Earth's Atmosphere?
- That pressure does not just go down, it
presses on all surfaces.
- Imagine a square on your belly, 10" x 10"
(100 in2).
- There would be a force of 14.7 lbs/in2
x 100 in2 = 1470 lbs (nearly 3/4 of a ton)
- Why don't we go flying backwards
then? Because there's an equal and opposite force on
your backside pushing in the other direction.
- Why don't we get squished, then? Two
related answers:
- Liquids and solids that make up our
bodies are incompressible.
- There is an equal and opposite outwards
pressure in our bodies.
- What happens to that pressure as we rise
higher and higher?
- As we rise, we get ABOVE some of the
atmosphere, so the air above us is less heavy.
- Therefore the pressure decreases as you
rise (see figure below left).
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Some things to note about this diagram:
- 50% of all the atmosphere lies below about
5.5 km altitude
- At an altitude of 11 km (roughly 35,000 ft,
the altitude that WWII (non-pressurized) aircraft flew at from
1939-1945), the air pressure is <30% of sea level air
pressure. If you tried to breath at those altitudes,
you'd quickly fall unconscious and die. Many of our fathers, grandfathers,
and (in some cases) great-grandfathers were fliers in
WWII. In order to stay conscious and alive,
they HAD to breath oxygen continuously. Our ancestors
not only flew at those altitudes, but fought at those
altitudes. Today, we comfortably fly in pressurized jet
airliners at that altitude without even thinking about it.
- Note that in the graph on the right, of water
pressure under the sea, decreases as you come up, for the same
reason that air pressure decreases as you rise: the
weight of the overlying fluid decreases as you get above the
fluid below.
- Water pressure decreases as you come up (or
increases as you go down) by 1 atm (i.e 14.7 lbs/in2)
about every 10
meters, in a straight line,
- because a 1 in2 column of water
10 meters long weighs 14.7 lbs.
- Pressure is 1 atm at surface because of air
pressure at sea level.
- But there's a difference in how air pressure
decreases as you go up.
- Note that the higher you go in the atmosphere,
the more slowly air pressure decreases for a given
increase in elevation.
- From sea level to 2 km, air pressure
decreases by about 200 mB.
- But if you rise 2 km from 8 to 10 km, air
pressure decreases by less than 100 mB.
- To get a 200 mB decrease, you'd need to rise
nearly to 14 km, a 3x greater increase in elevation than
from sea level.
- But as you rise in the ocean, the water
pressure decreases by exactly the same amount for a given
rise.
- Why? Because air (a gas) is
compressible and expandable. And as the pressure decreases,
the air expands and its density decreases.
- Water (a liquid) is not compressible.
And it stays at the same volume no matter the pressure, so
the density stays constant.
- So as you go higher and higher, you have to
go over greater and greater thicknesses of air to lose the
same amount of pressure.
- The curve of air pressure to altitude never
reaches zero pressure.
- The net result of this is that there is NO TOP
OF THE ATMOSPHERE.
- Instead, the atmosphere merges gradually with
space. There is no hard boundary.
- Any boundary between "atmosphere" and "space"
is arbitrary.
- NASA and the FAA set it at 100 km, about 62
miles high.
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Structure of Atmosphere:
Based on how temperature changes. Know the various
layers.
- Thermosphere:
Temperature increases as height increases.
- Mesopause (~80 km high)
- Mesosphere:
Temperature decreases as height increases.
- Stratopause (~47km high)
- Stratosphere (Ozone Layer is here): Temperature increases as height increases.
- Tropopause (10 km high)
- Troposphere (Weather is here): Temperature
decreases as height increases.
First of all, how do we know this? By sending
balloons and rockets up into the atmosphere and measuring
temperature. We can SEE that temperature decreases as we
rise in the Troposphere, because mountains are "snow
capped". Not because it only snows on the tops of mountains,
but because it is only cold enough for the snow to stay frozen
there. Lower down, the snow melts.
Note also the temperature at about 11km (where we previously
looked at air pressure being <30% of sea level pressure, and
where our ancestors flew during WWII). The temperature is
around -70oF! This is why, if you ever see a
WWII-era movie about aviation ("12 O'Clock High" is one of the
most well-known ones, but more modern ones like "Pearl Harbor",
"Red Tails", "Tuskeegee Airmen", "Midway", or "Memphis Bell"
also), the pilots and crews of fighters and bombers wear very
heavy clothing.
The second question you might have looking at this is: WHY do
the temperatures change in the way that we see?
Also see: https://climate.ncsu.edu/edu/Structure
- Troposphere: decreasing
temperatures as elevation increases.
- Another way of asking this is, WHY is the
surface of the earth warm?
- The answer, of course, is that it's heated
by the Sun.
- The Earth's atmosphere is largely
transparent to radiation from the Sun.
- That radiation comes down, hits the earth,
is (partly) absorbed, and heats the ground.
- This heats the atmosphere lying next to the
ground (known as "sensible heating").
- So as you move away from the surface, you're
farther from the source of heating, and temperature
decreases.
- Also, as warm air rises, it expands and
cools. This decrease in temperature is known as the
"adiabatic lapse rate" and is about 10oC/km in
the Troposphere. This decrease in temperature occurs
without any change in heat energy.
- Stratosphere: increasing temperatures as elevation increases.
- Mesosphere: decreasing temperatures as elevation increases.
- We can combine the 2 observations above and
note: Temperature reaches a maximum in the Stratopause.
Why?
- The short answer is: The Ozone Layer
- What does this mean? Look at the
figure below.
- When ultraviolet (UV) light from the Sun
hits an oxygen molecule (O2), it breaks it into 2
extremely (and dangerously) reactive individual oxygen
atoms.
- These oxygen atoms immediately recombine
with any available oxygen molecules, to produce a molecule
with three oxygen atoms That molecule (O3)
is known as "Ozone".
- When UV light encounters an Ozone molecule,
it is absorbed by Ozone. We can say that Ozone is
"opaque" to UV light.
- Anything that absorbs energy (like UV light
absorbed by Ozone) will warm up. So the air warms up.
- But note in the "Structure of the
Atmosphere" diagram, that the altitude of
maximum heating (the Stratopause) is significantly
higher than the layer of maximum Ozone.
Why is that?
- As UV comes DOWN through the
atmosphere, it is, bit by bit, absorbed by Ozone. So
the amount of UV available for heating decreases, and by the
time it reaches the maximum Ozone, there's only a little UV,
so a small amount of heating.
- As you go UP in the atmosphere, the
amount of air decreases, so there's less and less oxygen
available to be turned into Ozone, which means that there
will be less absorption of UV and less heating.
- The Stratopause, where there
is a temperature maximum, is the location where there is
enough Ozone to effectively absorb UV, and enough UV to
cause maximum heating.
- Above that point, there's not enough Ozone
to trap UV, so temperatures cool as you go up into the
Mesosphere.
- Below that point, there's not enough UV to
cause a lot of heating. So temperatures cool as you
go down into the Stratosphere.
- Finally, note that as you go up from the Mesopause
into the Thermosphere, temperatures again increase
with increasing altitude. Why?
- Note the altitudes here - we transition into
"space" as defined by NASA and the FAA.
- While this is not a "perfect" vacuum, the
pressures here are extremely low, and would be considered a
pure vacuum nearly anywhere on Earth.
- There are very few molecules and atoms of
gas here, but they are exposed to the full force of the
Sun's energy, so they are accelerated to very high speeds,
which means very high temperatures.
- That said, since the atoms and molecules are
so widely dispersed, there is little energy out there, even
if the temperatures are high. It is similar to 4th of
July sparklers, whose sparkles are very hot but so small
that they are relatively harmless.
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The next thing to consider is
the Composition of Atmosphere:
Air: a gas
Click on the name of each
gas to learn how it got there.
Click on the the percentage for additional information
about each gas.
&
- as of the late 1990s. As
of 2013, Methane has increased to 253% of preindustrial levels.
To be current, I really have to update these values almost every
year.
Note: please read all links
in the chart above (it's really only 2 web pages).
Ozone - O3
Problem with CFCs: destroy Ozone:
2O3 + CFC
==> 3O2 + CFC
CFCs are catalysts, and destroy 1000s of ozone
molecules before natural processes destroy the CFC
molecules. This has helped create the "Ozone Hole" in the
Antarctic and to a lesser extent, the Arctic.
(For
more information, click here!)
Radiation
Balance in Atmosphere (See your
textbook as well):
Radiation: The Spectrum:
Transparency of the Earth's Atmosphere.
Electromagnetic Radiation:
- Charged particles (electrons mostly) vibrate,
- causing fluctuating electric and magnetic
fields,
- which propagate outwards at the "speed of
light".
- This is "electromagnetic radiation", AKA
"light"
- The faster they vibrate, the higher the
frequency and the more energetic the waves.
- Gamma rays (highest
frequency (shortest wavelength))
- Then: Xrays,
- Ultraviolet
- Visible light:
- Violet
- Blue
- Green
- Yellow
- Orange
- Red
- Infrared (Most atoms on the surface of the
earth vibrate fast enough for these to be given off)
- Microwaves
- Radio waves (lowest frequency, longest
wavelength)
From the Sun:
- What
kind is most abundant?
- This makes a lot of sense:
- Our eyes are adapted to use the most
abundant light from the sun.
- If our sun gave off a lot of radio energy,
we might expect to have little radar dishes instead of
eyeballs.
- in contrast, UV (ultraviolet) light is shorter
wavelength,
- and IR (infrared) is longer wavelength than
visible light.
- And both are given off less by the sun than
visible light.
Of 100% of incoming light:
-
(from Science Direct)
- 30% is reflected (the albedo):
- 70% is absorbed:
- 19% by clouds and atmosphere
- 16% absorbed by greenhouse gases and dust
- 3% absorbed by clouds
- 51% by land and ocean:
- 21% eventually released as infrared (IR)
from surface (due to heating of surface)
- 7% released as "sensible heat" by
conduction into atmosphere
- 23 released as "latent heat" by
evaporation of water into atmosphere
- Of the 51% absorbed by land and ocean and
19% absorbed by clouds and atmosphere (70%):
- Only 6% IR makes it to space directly from
the surface
- 38% is emitted out to space as IR from greenhouse gases in
the atmosphere
- This means that IR is absorbed by
greenhouse gasses in the atmosphere,
- which causes these gases to warm,
- in turn releasing IR in all
directions,including back to the earth.
- The IR that is released BACK to the
earth, warms it again, increasing global temperatures.
- 26% is emitted out to space as IR from
clouds
The light energy absorbed by land and ocean causes
them to warm up, leading to the emission of long wave (IR)
radiation. This radiation is absorbed by CO2, H2O, CH4, N2O,
Ozone, and CFCs ("Greenhouse Gases"), which radiate back some of
the energy to the earth again, rewarming it. This absorption
and re-radiation of IR is what is known as the "Greenhouse
Effect".
Why do we get seasons? - due to tilt of the earth:
(See your textbook for a more detailed
explanation)
Air circulation - depends on changes in
temperature:
- Heat air
- Temperature rises
- Molecules move faster
- Gas expands
- Density decreases
- Air rises
Troposphere Lapse Rate ~6o C/km of
altitude - this is the "environmental" (actual) lapse rate you
actually experience if you go up in the altitude.
If you raise a parcel of air:
- expansion of air
- adiabatic cooling
- adiabatic lapse rate (may be different from
environmental lapse rate)
Examples:
Altitude:
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Temperature if Environmental
(actual) Lapse Rate = 12oC/km
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Temperature if Adiabatic Lapse
Rate = 10oC/km
|
What happens if the air rises
up 1 km?
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3 km
|
4oC
|
10oC
|
It's warmer than the surrounding
air.
|
2 km
|
16oC
|
20oC
|
It's warmer than the surrounding
air.
|
1 km
|
28oC
|
30oC
|
It's warmer than the surrounding
air.
|
0 km (sea level)
|
40oC
|
40oC
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Result: Unstable air mass (because the warm
air which is adiabatically cooling as it rises and expands is
still warmer than the surrounding air.
Altitude:
|
Temperature if Environmental
(actual) Lapse Rate = 5oC/km
|
Temperature if Adiabatic Lapse
Rate = 10oC/km
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What happens if the air rises up 1
km?
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3 km
|
5oC
|
-10oC
|
It's colder
than the surrounding air.
|
2 km
|
10oC
|
0oC
|
It's colder
than the surrounding air.
|
1 km
|
15oC
|
10oC
|
It's colder
than the surrounding air.
|
0 km (sea
level)
|
20oC
|
20oC
|
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Result: Stable
air mass (because the warm air which is adiabatically cooling as
it rises and expands is colder than the surrounding air.
How do we lift Stable air? We can do it
when a wind blows over mountains; it falls right back down
again!: