Wed., Apr. 11, 2012
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April Smith and the Great Picture Show were featured before class
today (I heard one of their songs "Colors" on a
Lowes commercial on TV). My Ipod has been acting a little
strangely and picking songs in random order. So I'm not sure
which of these you heard ("Movie Loves a Screen",
"Terrible Things",
"Can't Say No",
or
"Wow and Flutter")
The "Recent Climate Events" 1S1P reports, the Stability worksheet,
and the In-class Optional Assignment from last Friday were all returned
today. A new 1S1P Bonus
Assignment topic has also been added.
I might have scared a few students when they saw Pt. 1 of the Quiz #4 Study Guide appear
online. Quiz #4 is still a couple of weeks away (it's on Wed.,
Apr. 25).
Here's an idea of what we'll cover in class today.
We'll
look
at the development of a thermal circulation.
Differences
in
temperature like you might find between a coast and
the ocean or between a city and the surrounding country side can create
horizontal pressure differences. The horizontal pressure gradient can
then produce a wind flow pattern known as a thermal circulation.
When dealing with these usually small scale circulations, the
pressure gradient force is often so much stronger than the Coriolis
force
that the
Coriolis force can be ignored.
We will learn how thermal
circulations develop and then apply to concept to the earth as a
whole
in order to understand large global scale pressure and wind
patterns. You really can't
ignore the Coriolis force in a situation like that so the concept is
not really applicable on that scale. But much of what it predicts
is actually found in the real world. That's why we'll cover and
study this topic.
Thermal
Circulations
You'll find this
discussed on p. 131 in the photocopied Class Notes.
The figures below are more
carefully drawn versions of what is in the ClassNotes.
We've
situated
ourselves
along
a
sea
coast. There aren't any temperature differences yet in this
picture (both the ocean and the land are shaded green), so the pressure
at the ground and above the
ground are the same over the land and over the ocean.
A beach will often become much
warmer than the
nearby
ocean during
the day (the sand gets hot enough that it is painful to walk across in
bare feet). The ocean is much harder to warm and won't change
temperature much during the day. The warm ground will warm the
air above. Pressure
decreases more slowly as you move upward through warm low density
air (this is something we covered early in the semester). As you
move from the ground to the level of the green line
in the picture above pressure decreases 90 mb in the warm air and a
little more, 100 mb, in the cooler denser air over the ocean.
Here's another way of figuring out
what happens. The warm air
expands pushing the 900 mb pressure level to a higher level than it
would normally be found. 910 mb pressure
from a little lower altitude moves in to take its place.
The temperature differences at the
ground have created an upper
level pressure
gradient (pressure difference), higher pressure (910 mb) on the left
and lower pressure (900 mb) on the right. The resulting pressure
gradient force (PGF) causes air to start to blow from left to right.
The upper level winds (which remove air from the left side of the
picture and add it to the right) will then affect the surface pressure
pattern.
Air leaving the left side of the
picture
will lower the surface pressure (from 1000 mb to 990 mb). Adding
air aloft to the right side of the picture will increase the surface
pressure (from 1000 mb to 1010 mb). Surface winds will start to
blow from right to left.
You can complete the circulation
loop by adding rising air
above the
surface low pressure at left and sinking air above the surface high at
right. The surface winds which blow from the ocean onto land are
called a sea breeze (the name tells you where the winds come
from). Since this air is likely to be moist, cloud formation is
likely when the air rises over the warm ground. Rising air
expands and cools. If you cool moist air to its dew point, clouds
form.
Here's a short cut that will allow you to quickly figure the
directions of the winds in a
thermal
circulation without going through a long-winded development like we
just done. Just
remember
that warm air rises
Draw
in
a
rising
air
arrow
above
the
warm
part
of
the
picture, then complete the loop.
At night the ground cools more quickly than the ocean and becomes
colder than the water (the water temperature didn't change at all in
the picture below). Rising air is found over the ocean
water because it is warmer than the land. The thermal circulation
pattern reverses
direction. Surface winds blow from the land out over the
ocean. This is referred to as a land breeze.
Clouds now form out over the ocean.
Here
are
some
additional
examples
of
thermal
circulations
or
large
scale
circulations
that
resemble
thermal circulations.
Cities are often warmer than the
surrounding
countryside,
especially at night. This is referred to as the urban heat island
effect. This difference in temperature can create a
"country breeze." This will sometimes carry pollutants
from a factory outside the city back into the city or odors from a
sewer treatment plant outside of town back into town.
The Asian monsoon is a large scale circulation
pattern and is much more complex than a simple thermal
circulation. However you can
use the thermal circulation concept to get a general understanding of
what to expect at different times of the year. Before
looking at that let's be clear about the meaning of the term monsoon.
Monsoon just refers to a seasonal change in the direction of the
prevailing winds. In southern Arizona it is often used
(incorrectly) to just mean a thunderstorm.
In the summer land masses in India
and SE
Asia
become warmer than the
oceans
nearby. Surface low pressure forms over the land, moist winds
blow from the ocean onshore, and very large amounts of rain can
follow. A map view (top view) is shown at left, a
crossectional view is shown at right.
The winds change
directions in the
winter when the
land becomes colder
than the ocean.
You can
also use the thermal circulation to understand some of the basic
features of the El Nino phenomenon (you find a discussion of the El
Nino on pps 135-139 in the photocopied Classnotes).
First here is what conditions look like in the tropical Pacific
Ocean
in non-El Nino years (top and side views again)
Cold ocean currents
along the west coasts of N. America and S.
American normally converge at the equator and begin to flow westward
(see top view above). As the water travels westward it
warms. Some of the warmest sea surface waters on earth are
normally found
in the western Tropical Pacific (this is also where hurricane are most
frequent). A temperature gradient becomes
established between the W. and E. ends of the tropical Pacific. The
crossectional view above shows the normal temperature and circulation
pattern found in the equatorial Pacific Ocean. You would
find surface high pressure in the east and low pressure in the
west. Note that the wind circulation pattern is the same as the
simple thermal circulation we studied above.
During a La Nina event, waters in the Eastern Pacific are even
colder than normal. This generally produces drier than normal
conditions during the winter in the desert SW. This was the case
last winter and La Nina conditions are again in effect this
winter. You can read more about La Nina here.
Every few years El Nino conditions occur and the cold
currents don't
make it to the
Equator. Warm water is carried from the western Pacific to the
eastern Pacific. The temperature and pressure basically reverses
itself.
Now surface high
pressure is found in the west and surface low
pressure and rising air is found in the E. Pacific (the reversal in the
surface pressure pattern is referred to as the southern
oscillation). Indonesia and Australia often experience drought
conditions (and devastating wildfires) during El Nino years. In
the desert SW we expect
slightly wetter than normal conditions (perhaps 20% wetter than
normal). Wetter conditions are also found in California and in
the SE US.
Here's a map showing the effects of El Nino and La Nina conditions
on winter weather in N. America (source).
This map wasn't
shown in class.
In
the desert SW we expect
slightly wetter than normal conditions (perhaps 20% wetter than
normal) during an El Nino event (upper portion of the figure).
Wetter conditions are also found in California and in
the SE US. La Nina generally means
drier than normal weather in the desert SW.
The second main topic
of the day: using
the
thermal
circulation
idea
to
learn
something
about
global
scale
pressure
and
wind
patterns
on the
earth. Ordinarily you couldn't apply a small scale phenomena like
a thermal circulation to the much larger global scale. However if
we make some simplifying assumptions, particularly if we assume that
the earth doesn't rotate or only rotates slowly, we can ignore the
Coriolis force and a thermal circulation could become established.
Some additional simplifications are also made and are listed below
(p.
133 in the photocopied Classnotes). The figures are more
carefully drawn versions of what was done in class.
Because the earth isn't tilted, the
incoming sunlight
shines
on the earth most directly at
the
equator. The equator will become hotter than the poles. By
allowing
the
earth
to
rotate
slowly
we
spread
this
warmth
out
in
a
belt
that
circles
the
globe
at the equator rather than concentrating it in a
spot on
the side of the earth facing the sun. Because the
earth is of uniform composition there aren't any temperature
differences created between oceans and continents.
You can see the wind
circulation pattern that would develop. You'd find rising
air at the equator (the "warm air rises" shortcut rule again).
Upper level winds would blow from equator toward the N and S
Poles. Winds would converge and sink at the poles. Surface
winds would blow from the poles toward the equator. The term one
cell
just refers to the single complete
loop
in each hemisphere.
Next we will remove the assumption concerning the rotation of the
earth. We won't be able to ignore the Coriolis force now.
Here's what a computer would
predict you would now see
on
the earth. The temperature pattern remains the same and things
are pretty much the same at the equator in the
three cell and one cell models: surface low pressure and rising
air. At
upper levels the winds begin to blow from the equator toward the
poles. Once headed toward the poles the upper
level winds are deflected by the Coriolis force.
There end up being three closed loops in the northern and in the
southern hemispheres. There are surface belts of low
pressure
at the equator (the equatorial low)
and at 60 degrees latitude (the subpolar
low). There are belts of high pressure (the subtropical high) at 30
latitude and high pressure centers at the two poles (the polar highs).
On Friday we will look at the 3-cell model surface features
(pressure belts
and
winds) in a little more detail because
some of what is predicted, even with the unrealistic assumptions, is
actually found on the earth.