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Principles of terrestrial ecosystem ecology.pdf

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Hadley cell<br />

Hadley cell<br />

Ferrell cell<br />

Ferrell cell<br />

Westerlies<br />

NE tradewinds<br />

SE tradewinds<br />

Westerlies<br />

Polar cell<br />

ITCZ<br />

lation cell in the Northern Hemisphere and<br />

another in the Southern Hemisphere, driven by<br />

atmospheric heating and uplift at the equator<br />

and subsidence at the poles. Based on observations,<br />

Ferrell proposed in 1865 the conceptual<br />

model that we still use today, although the<br />

actual dynamics are much more complex. This<br />

model describes atmospheric circulation as a<br />

series <strong>of</strong> three circulation cells in each hemisphere.<br />

(1) The Hadley cell is driven by expansion<br />

and uplift <strong>of</strong> equatorial air. (2) The polar<br />

cell is driven by subsidence <strong>of</strong> cold converging<br />

air at the poles. (3) The intermediate Ferrell cell<br />

is driven indirectly by dynamical processes (Fig.<br />

Cold subsiding air<br />

Cold subsiding air<br />

60 o<br />

Subtropical high pressure<br />

Polar cell<br />

Polar front<br />

Subtropical high pressure<br />

Polar front<br />

Figure 2.6. Earth’s latitudinal atmospheric circulations<br />

are driven by rising air at the equator and subsiding<br />

air at the poles. These forces and the Coriolis<br />

forces produce three major cells <strong>of</strong> vertical atmospheric<br />

circulation (Hadley, Ferrell, and polar cells).<br />

Air warms and rises at the equator due to intense<br />

heating. After reaching the tropopause, the equatorial<br />

air moves poleward to about 30° N and S latitudes,<br />

where it descends and either returns to the<br />

equator, forming the Hadley cell, or moves poleward.<br />

Cold dense air at the poles subsides and moves<br />

toward the equator until it encounters polewardmoving<br />

air at about 60° latitude. There the air rises<br />

30 o<br />

The Atmospheric System 25<br />

Warm rising air<br />

0 o<br />

Cold subsiding air<br />

Warm rising air<br />

Warm<br />

rising<br />

air<br />

Cold subsiding air<br />

and moves either poleward to replace air that has<br />

subsided at the poles (the polar cell) or moves<br />

toward the equator to form the Ferrell cell. Also<br />

shown are the horizontal patterns <strong>of</strong> atmospheric circulation,<br />

consisting <strong>of</strong> the prevailing surface winds<br />

(the easterly trade winds in the tropics and the<br />

westerlies in the temperate zones). The boundaries<br />

between these zones are either low-pressure zones<br />

<strong>of</strong> rising air (the intertropical conversion zone,<br />

ITCZ, and the polar front) or high-pressure zones <strong>of</strong><br />

subsiding air (the subtropical high pressure belt and<br />

the poles).<br />

2.6). The Ferrell cell is actually the long-term<br />

average transport caused by weather systems in<br />

the mid-latitudes rather than a stable permanent<br />

atmospheric feature. The chaotic motion<br />

<strong>of</strong> these mid-latitude weather systems creates a<br />

net poleward transport <strong>of</strong> heat. These three<br />

cells subdivide the atmosphere into three distinct<br />

circulations: tropical air masses between<br />

the equator and 30° N and S, temperate air<br />

masses between 30 and 60° N and S, and polar<br />

air masses between 60° N and S and the poles<br />

(Fig. 2.6). The latitudinal location <strong>of</strong> these<br />

cells moves seasonally in response to latitudinal<br />

changes in surface heating by the sun.

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