Title: General Circulation
1General Circulation Thermal Wind
- April 14, 2009
- AOS 101-302
2General Circulation
- What is the global picture?
- The average flow on the globe...
3General Circulation Hadley Cell
- Thermally-driven convection
- Warm air rises and cold air sinks, creating
circulation
4General Circulation 3 Cells
- Hadley Thermally driven circulation confined to
tropics - Ferrell Mid-latitude circulation cell
(subtropics to polar front) - Polar Sinking air at the poles
5General Circulation Winds
- Trade Winds Surface easterly winds diverging
from subtropical Highs and converging near the
Equator - Westerlies Diverge from subtropical Highs
converge toward polar front - Polar Easterlies Converge along the polar front
6General Circulation Sea Level Pressure
- Low Pressure (converging air!)
- ITCZ (Intertropical convergence zone), near the
equator - Subpolar Lows along the polar front, near 60
- High Pressure (diverging air!)
- Subtropical Highs near 30 (warm dry)
- Polar High at the pole (cold dry)
7General Circulation Climate
- Deserts at subtropical highs (High sinking
air!) - Rainforests near ITCZ (Low rising air
clouds!) - Polar regions are deserts and receive very little
precipitation each year (High sinking air!)
8General Circulation Jet Streams
9Pressure
- Pressure is the weight of air molecules ABOVE you
- Pressure decreases with altitude because there
are less air molecules above you as your rise - As a result of pressure changes, Temperature,
Density, and Volume change too as you rise
http//www.srh.noaa.gov/jetstream//atmos/images/mb
_heights.jpg
10Thickness...
11- Start with a column of air.
12- The base of this column is at the surface, so
lets say its pressure is about 1000 mb
1000 mb
13- The top of this column is quite highlets say
that its pressure is 500 mb
500 mb
1000 mb
14- This column has some thickness it is some
distance between 1000 mb and 500 mb
500 mb
1000 mb
15500 mb
- If we heat the column of air, it will expand,
warm air is less dense - The thickness of the column will increase
- 500mb is now farther from the ground
1000 mb
Warmer
16- If we cool the column of air, it will shrink,
cool air is more dense - The thickness of the column will decrease
- 500mb is now closer to the ground
500 mb
1000 mb
Colder
17Thickness
- In fact, temperature is the ONLY factor in the
atmosphere that determines the thickness of a
layer - It wouldnt have mattered which pressure we had
chosen. They are all higher above the ground
when it is warmer.
18Thickness
- In fact, temperature is the ONLY factor in the
atmosphere that determines the thickness of a
layer - It wouldnt have mattered which pressure we had
chosen. They are all higher above the ground
when it is warmer. - which is what this figure is trying to show
19Thickness
- At the poles, 700 mb is quite low to the ground
- These layers are not very thick
- In the tropics, 700mb is much higher above the
ground - See how thick these layers are
20General Circulation!
Lets think about what thickness means near a
polar front, where cold air and warm air are
meeting
21This is a cross section of the atmosphere
North COLD
South WARM
22Cold air is coming from the north. This air
comes from the polar vortex near the North Pole
North COLD
South WARM
23Warm air is coming from the south. This air
comes from the subtropical high near 30N
North COLD
South WARM
24These winds meet at the polar front (a strong
temperature gradient)
POLAR FRONT
North COLD
South WARM
25Now, think about what we just learned about how
temperature controls the THICKNESS of the
atmosphere
POLAR FRONT
North COLD
South WARM
26On the warm side of the front, pressure levels
like 500mb and 400mb are going to be very high
above the ground
400mb
500mb
POLAR FRONT
North COLD
South WARM
27On the cold side of the front, pressure levels
like 500mb and 400mb are going to be very low to
the ground
400mb
500mb
400mb
500mb
POLAR FRONT
North COLD
South WARM
28Above the front, thickness of atmosphere changes
rapidly
400mb
500mb
400mb
500mb
POLAR FRONT
North COLD
South WARM
29Now, what about the PGF above the front?
400mb
500mb
400mb
500mb
POLAR FRONT
North COLD
South WARM
30Lets draw a line between the cold side of the
front and the warm side
400mb
500mb
A
B
400mb
500mb
POLAR FRONT
North COLD
South WARM
31What is the pressure at point A?
400mb
500mb
A
B
400mb
500mb
POLAR FRONT
North COLD
South WARM
32The pressure at point A is less than 400mb, since
it is higher than the 400mb isobar on this plot.
Lets estimate the pressure as 300mb
400mb
500mb
A
B
300mb
400mb
500mb
POLAR FRONT
North COLD
South WARM
33What is the pressure at point B?
400mb
500mb
A
B
300mb
400mb
500mb
POLAR FRONT
North COLD
South WARM
34The pressure at point B is more than 500mb, since
it is lower than the 500mb isobar on this plot.
Lets estimate the pressure as 600mb
400mb
500mb
A
B
300mb
600mb
400mb
500mb
POLAR FRONT
North COLD
South WARM
35The pressure gradient force between point B A
is HUGE Therefore, all along the polar front,
there will be a strong pressure gradient force
aloft, pushing northward
400mb
PGF
500mb
A
B
300mb
600mb
400mb
500mb
POLAR FRONT
North COLD
South WARM
36- Strong PGF is
- Aloft (above the surface)
- Above the Polar Front (strong temperature
gradient!) - PGF pushes to the north (in the Northern
Hemisphere) - How does this cause the midlatitude jet stream?
37Midlatitude Jet Stream
- Suppose we have a polar front at the surface
- This purple line is the polar front at the
surface - As well learn, this is NOT how fronts are
correctly drawn, but it will work for now
38Midlatitude Jet Stream
- All along the front, there is a strong pressure
gradient force pushing northward
39Midlatitude Jet Stream
- Winds aloft are in geostrophic balance
40Midlatitude Jet Stream
- So the wind will be accelerated North by the PGF,
then turned to the East by the Coriolis effect - The true wind will be a WESTERLY wind, directly
above the polar front
41Midlatitude Jet Stream
The same diagram from a different angle
- Here is the polar front at the surface
42Midlatitude Jet Stream
- Remember, its a polar front because it is where
warm air from the south meets cold air from the
north.
43Midlatitude Jet Stream
- The midlatitude jet stream is found directly
above the polar front.
44Midlatitude Jet Stream
- The (Northern Hemisphere) Midlatitude Jet Stream
is found directly above the polar front, with
cold air to the LEFT of the flow - This is because of the changes in thickness
associated with the polar front - This same relationship exists near ANY front
(temperature gradient) known as the THERMAL WIND
RELATIONSHIP
45Large temperature gradients at the surface
correspond to strong winds aloft!
46Large temperature gradients at the surface
correspond to strong winds aloft!
47Thermal Wind
- Upper-level winds will be much stronger than
low-level winds (i.e. thermal wind will be very
close to upper-level wind) - Equal to the SHEAR of the geostrophic wind (i.e.
change of geostrophic wind with height) - Not an actual wind
- Stronger temperature gradients imply stronger
thermal wind - Blows along thickness contours with (low
thickness) air to the left
Thermal Wind
Lower Level Geostrophic Wind
Upper level geostrophic wind
48Thermal Wind
VT
Upper level geostrophic wind
Lower Level Geostrophic Wind
49Thermal Wind
COLD
5540 m
VT
5600 m
Upper level geostrophic wind
5660 m
Lower Level Geostrophic Wind
WARM
50Backing Veering
If winds rotate clockwise from lower level to
upper-level ? veering!
Thermal Wind
Lower level Geostrophic winds
Upper Level Geostrophic wind
51Backing Veering
If winds rotate clockwise from lower level to
upper-level ? veering!
If winds rotate counter-clockwise with height ?
backing!
Upper Level Geostrophic Wind
Thermal Wind
Lower level Geostrophic winds
Lower Level Geostrophic Wind
Upper Level Geostrophic wind
Thermal Wind
52Backing Veering
If winds rotate clockwise from lower level to
upper-level ? veering!
If winds rotate counter-clockwise with height ?
backing!
Upper Level Geostrophic Wind
Thermal Wind
Lower level Geostrophic winds
Lower Level Geostrophic Wind
Upper Level Geostrophic wind
Thermal Wind
53Backing Veering
If winds rotate clockwise from lower level to
upper-level ? veering!
If winds rotate counter-clockwise with height ?
backing!
Upper Level Geostrophic Wind
Thermal Wind
Lower level Geostrophic winds
Lower Level Geostrophic Wind
Upper Level Geostrophic wind
Thermal Wind
Warm Air Advection!
Cold Air Advection!
54Some terminology.
55Fronts Symbols(point in direction of front
movement)
COLD
WARM
OCCLUDED
STATIONARY
56Warm Front
WARM
COOL
- Gradual Slope
- Stratiform rain
- Long lasting light rain
- Occurs on cool side of front
- Temperature increases prior to frontal passage
- Wind becomes southerly after passage
57Cold Front
WARM
COOL
- Much Steeper Slope
- More intense (convective) rain
- Thunderstorms for a shorter period
- occurs on warm side of front
- Temperature decreases after frontal passage
- Wind becomes northerly after passage
58Frontal-Cyclone Structure
Cool Air
L
Lighter Rain
Cold Air
Warm Air
Heavier Rain
59Finding a Front
- Temperature (Dewpoint) Gradient
- Change in wind direction
- Converging winds at the front
- Kink or trough in isobars (lower pressure)
- Banded precipitation
60Upper-level terminology
- Trough area of lower heights
- Ridge area of higher heights
L
H
61Geopotential Height
The height of a pressure surface above ground is
analogous to the pressure. As an example, a low
height of the 500 mb surface is analogous to
lower pressure. This will be very important when
we analyze upper tropospheric data.
Figure A 3-dimensional representation of the
height of the 500 mb surface (in meters)
62Hydrostatic Balance
- Pressure decreases with height
- Thus we have a vertical pressure gradient force
pointing...Upward! - This is counteracted by the gravitational force,
which points downward - This balance is called Hydrostatic Balance
- Often we take this to be the case in our
atmosphere