
Apago PDF Enhancer
North
Pole
Westerlies
Westerlies
60°S
30°S
30°N
60°N
0°
Northeast trades
Southeast trades
Equatorial
low precipitation
high precipitation
Figure 59.3
Global patterns of atmospheric circulation.
The diagram shows the patterns of air circulation that prevail on
average over weeks and months of time (on any one day the patterns
might be dramatically different from these average patterns). Rising
air that is cooled creates bands of relatively high precipitation near
the equator and at latitudes near 60°N and 60°S. Air that has lost
most of its moisture at high altitudes tends to descend to the surface
of the Earth at latitudes near 30°N and 30°S, creating bands of
relatively low precipitation. The red arrows show the winds blowing
at the surface of the Earth; the blue arrows show the direction the
winds blow at high altitude. The winds travel in curved paths
relative to the Earth’s surface because the Earth is rotating on its
axis under them (the Coriolis effect). A terminological problem to
recognize is that the formal names given to winds refer to the
directions from which they come, rather than the directions toward
which they go; thus, the winds between 30° and 60° are called
Westerlies because they come out of the west. Unfortunately,
oceanographers use the opposite approach, naming water currents
for the directions in which they go.
are affected by the spinning of the Earth on its axis; we discuss
this effect shortly.
For complex reasons, the air circulating up from the equa-
tor and away at high altitudes in both hemispheres tends to cir-
culate back down to the surface of the Earth at about 30° of
latitude, both north and south (see figure 59.3). During the
course of this movement, the moisture content of the air changes
radically because of the changes in temperature the air under-
goes. Cooling dramatically decreases air’s ability to hold water
vapor. Consequently, much of the water vapor in the air rising
from the equator condenses to form clouds and rain as the air
moves upward. This rain falls in the latitudes near the equator,
latitudes that experience the greatest precipitation on Earth.
By the time the air starts to descend back to the Earth’s
surface at latitudes near 30°, it is cold and thus has lost most of
its water vapor. Although the air rewarms as it descends, it does
not gain much water vapor on the way down. Many of the
greatest deserts occur at latitudes near 30° because of the steady
descent of dry air to the surface at those latitudes. The Sahara
Desert is the most dramatic example.
The air that descends at latitudes near 30° flows only
partly toward the equator after reaching the surface of the
Earth. Some of it flows toward the poles, helping to give rise in
each hemisphere to winds that blow over the Earth’s surface
from 30° toward 60° latitude. At latitudes near 60° air tends to
rise from the surface toward high altitudes.
Inquiry question
?
Why is it hotter at latitudes near 0°?
The Coriolis effect
If Earth did not rotate on its axis, global air movements would
follow the simple patterns already described. Air currents—the
winds—move across a rotating surface, however. Because the
solid Earth rotates under the winds, the winds move in curved
paths across the surface, rather than straight paths. The curva-
ture of the paths of the winds due to Earth’s rotation is termed
the Coriolis effect, after the 19th-century French mathemati-
cian, Gaspard-Gustave Coriolis, who described it.
If you were standing on the North Pole, the Earth would
appear to be rotating counterclockwise on its axis, but if you
were at the South Pole, the Earth would appear to be rotating
clockwise. This property of a rotating sphere, that its direction
of rotation is opposite when viewed from its two poles, explains
why the direction of the Coriolis effect is opposite in the two
hemispheres. In the northern hemisphere, winds always curve
to the right of their direction of motion; in the southern hemi-
sphere, they always curve to the left.
The reason for these wind patterns is that the circumfer-
ence of a sphere, the Earth, changes with latitude. It is zero at
the poles and 38,000 km at the equator. Thus, land surface
speed changes from about 0 to 1500 km per hour going from
the poles to the equator. Air descending at 30° north latitude
may be going roughly the same speed as the land surface below
it. As it moves toward the equator, however, it is moving more
slowly than the surface below it, so it is deflected to its right in
the northern hemisphere and to its left in the southern
hemisphere. In other words, in both the northern and southern
surface at equatorial latitudes causes air to rise from the surface
to high in the atmosphere at these latitudes. This rising air is
typically rich with water vapor; one reason is that the moisture-
holding capacity of air increases when it is heated, and a second
reason is that the intense solar radiation at the equator provides
the heat needed for great quantities of water to evaporate. After
the warm, moist air rises from the surface (figure 59.3) , rising
air underneath it is pushed away from the equator at high alti-
tudes (above 10 km), to the north in the northern hemisphere
and to the south in the southern hemisphere. To take the place
of the rising air, cooler air flows toward the equator along the
surface from both the north and the south. These air move-
ments give rise to one of the major features of the global atmo-
spheric circulation: air flows toward the equator in both
hemispheres at the surface, rises at the equator, and flows away
from the equator at high altitudes. The exact patterns of flow
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part
VIII
Ecology and Behavior
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