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Chapter 8 Atmospheric Circulation and Pressure Distributions. George Hadley (1685-1768) proposed a simple circulation pattern called the single-cell model to describe the general movement of the atmosphere.

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Chapter 8 Atmospheric Circulation and Pressure Distributions

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Chapter 8 atmospheric circulation and pressure distributions

Chapter 8

Atmospheric Circulation

and

Pressure Distributions


Chapter 8 atmospheric circulation and pressure distributions

George Hadley (1685-1768) proposed a simple circulation pattern called the single-cell model to describe the general movement of the atmosphere.

In the single-cell model, air expands upward, diverges toward the poles, descends, and flows back toward the equator near the surface. Winds blowing east-to-west or west-to-east are referred to as zonal winds;

those moving north-to-south or

south-to-north are called meridional.


Chapter 8 atmospheric circulation and pressure distributions

The three-cell model

divides the circulation of each hemisphere into

three distinct cells:

the heat-driven Hadley cell that circulates air between the Tropics and subtropics,

a Ferrel cell in the middle latitudes, and a polar cell.


Chapter 8 atmospheric circulation and pressure distributions

Along the equator, strong solar heating causes air to expand upward and

diverge toward the poles, creating a zone of low pressure at the

equator called the equatorial low or the Intertropical Convergence Zone.

The ITCZ is the rainiest latitude zone in the world and is observable as

the band of convective clouds and showers extending from northern

South America into the Pacific on this satellite image.


Chapter 8 atmospheric circulation and pressure distributions

At about 20° to 30° latitude, air in the Hadley cell sinks toward

the surface to form the subtropical highs, large bands of

high surface pressure. Cloud formation is greatly suppressed

and desert conditions are common in the subtropics.

In the Northern Hemisphere, as the pressure gradient

force directs surface air from the subtropical highs to

the ITCZ, the weak Coriolis force deflects the air slightly

to the right to form the northeast trade winds.

In the Southern Hemisphere, the northward-moving air from

the subtropical high is deflected to the left

to create the southeast trade winds.


Chapter 8 atmospheric circulation and pressure distributions

Immediately flanking the Hadley cell in each hemisphere is the

Ferrel cell, which circulates air between the subtropical highs

and the subpolar lows, or areas of low pressure.

On the equatorial side of the Ferrel cell, air flowing poleward away

from the Northern Hemisphere subtropical high undergoes a substantial

deflection to the right, creating a wind belt called the westerlies.

In the Southern Hemisphere, the pressure gradient force propels the

air southward, but the Coriolis force deflects it to the left, producing

a zone of westerlies in that hemisphere as well.


Chapter 8 atmospheric circulation and pressure distributions

In the polar cells of the three-cell model, surface air moves

from the polar highs to the subpolar lows. Compared to

the poles, air at subpolar locations is slightly warmer,

resulting in low surface pressure and rising air.

Very cold conditions at the poles create

high surface pressure and low-level motion

toward the equator. In both hemispheres,

the Coriolis force turns the air to form

a zone of polar easterlies in the lower atmosphere.


Chapter 8 atmospheric circulation and pressure distributions

The real world is not covered by a series of belts that completely encircle

the globe. Instead, we find a number of alternating semi-permanent cells

of high and low pressure. Among the most prominent features in the

Northern Hemisphere during winter are the Aleutian and Icelandic Lows

over the Pacific and Atlantic Oceans, and the Siberian High over central Asia.


Chapter 8 atmospheric circulation and pressure distributions

In summer, the best-developed semi-permanent cells are the

Hawaiian and Bermuda-Azores Highs of the Pacific and Atlantic Oceans

and the Tibetan Low of southern Asia.


Chapter 8 atmospheric circulation and pressure distributions

The Sahel is a region of Africa bordering the southern Sahara Desert. During the summer (left), the ITCZ usually shifts northward and brings rain to the region. For much of the year,

the ITCZ is located south of the Sahel, and the region

receives little or no precipitation (right).


Chapter 8 atmospheric circulation and pressure distributions

Wind speeds generally increase with height between the surface and the

tropopause largely because pressure gradient force is typically stronger at

high altitudes. The surfaces representing the 900, 800, and 700 mb levels

all slant downward to the north, but not by the same amount. Higher surfaces

slope more steeply, which means that the pressure gradient force is greater.


Chapter 8 atmospheric circulation and pressure distributions

The polar front is a strongly sloping boundary between warm mid-latitude

air and cold polar air. Within the front, the slope of the pressure surfaces

increases greatly because of the abrupt horizontal change in temperature.

With steeply sloping pressure surfaces there is a strong pressure gradient force,

resulting in the polar jet stream situated above the polar front near the tropopause.


Chapter 8 atmospheric circulation and pressure distributions

Jet streams can be thought of as meandering “rivers” of air, usually 9 to 12 km

above sea level. Their wind speeds average about 180 km/hr in winter and

about half that in summer, though peak winds can exceed twice these values.

Nearer the equator is the subtropical jet stream, associated with the Hadley cell.

The subtropical jet stream can bring with it warm, humid conditions as seen above.


Chapter 8 atmospheric circulation and pressure distributions

This hypothetical drawing of the 500 mb surface reveals that heights decrease from south to north but also rise and fall through the ridges

and troughs. Vertical changes are highly exaggerated in the figure. Actual height changes are small compared to the size of the continent.


Chapter 8 atmospheric circulation and pressure distributions

Troughs occur in the middle troposphere where the 500 mb height contours dip equatorward. In the top map, positions 1–3 have the 500 mb level at 5610 m. Farther to the south, at positions 4–6, the 500 mb level is at 5640 m. In the bottom map, contour lines are in the same position over the East and West Coasts as they were up top, but shift equatorward over the central portion of the continent. Thus, positions 2 and 5 have lower pressure than the areas

east and west of them. The zone of lower pressure over the central part

of the continent is a trough.


Z 300 03 11 2008

Z 300-03/11-2008


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Snitt på tvers av jetstrømmen, syd for Grønland


Z 200 03 11 2008

Z 200-03/11-2008


Chapter 8 atmospheric circulation and pressure distributions

There are anywhere from three to seven Rossby waves or long waves

circling the globe, each with a particular wavelength and amplitude.

Rossby waves often remain in fixed positions, but also migrate west to east

and are capable of transporting warm air from subtropical regions

to high latitudes, or cold polar air to low latitudes.


Chapter 8 atmospheric circulation and pressure distributions

Ocean currents are horizontal movements of surface water that have an impact on the exchange of energy and moisture between the oceans and the lower atmosphere. Among these are the North Equatorial Current and the South Equatorial Current,which converge, creating the Equatorial Countercurrent. The warm Gulf Stream flows northeast tobecome the North Atlantic Drift and later the cold Canary Current as it turns southward. The cold Labrador Current flows south along the east coast

of Canada fed by the East and West Greenland Drift.


Chapter 8 atmospheric circulation and pressure distributions

Ocean currents are driven by winds in the lower atmosphere that exert a drag on the water at an angle 45° to the right (Northern Hemisphere) and continue to shift clockwise as their speed decreases. At a depth of about 100 m, the current approaches the opposite direction of the surface current and begins to die out in a pattern known as the Ekman spiral.


Chapter 8 atmospheric circulation and pressure distributions

Strong offshore winds along a coastal region sometimes

drag the warmer surface waters seaward, which

draws up cooler waters from below to take their place.

This process, called upwelling,

greatly influences sea surface temperatures

over the eastern portions of the major oceans.


Chapter 8 atmospheric circulation and pressure distributions

Features such as the Intertropical Convergence Zone, the

westerlies, and large Rossby waves exist on a global scale.

Smaller features, such as cyclones, anticyclones,

troughs, and ridges, exist at the synoptic scale,

covering hundreds or thousands of square kilometers.

Mesoscale events are on the order of tens of square

kilometers and last for periods as brief as half an hour.

The smallest exchanges of mass and energy

operate at the microscale.


Chapter 8 atmospheric circulation and pressure distributions

Monsoonrefers to the climatic pattern in which heavy precipitation alternates with hot, dry conditions on an annual basis due to the seasonal reversal in surface winds caused by an oscillation between high- and low-pressure cells. During winter (top), dry air flows southward from the Himalayas. When summer arrives (bottom) moist air is drawn northward from the equatorial oceans. Surface heating, convergence, and a strong orographic effect

cause heavy rains over the

southern part of the continent.


Chapter 8 atmospheric circulation and pressure distributions

Foehn is the generic name for synoptic scale winds that flow down

mountain slopes, warm by compression, and introduce hot, dry,

and clear conditions to the adjacent lowlands.

Winds warmed by compression that descend the eastern slopes of

the Rocky Mountains are called chinooks.

The Santa Ana winds of California, common in the fall and spring,

occur when high pressure develops over the Rocky Mountains.

Katabatic winds originate when air is locally chilled over a high-

elevation plateau and warmed by compression as it flows down slope.


Chapter 8 atmospheric circulation and pressure distributions

Along the coast during the daytime,

land surfaces warm more rapidly than the adjacent water (a), which causes the air column overlying the land to expand and rise upward (b). At a height of about 1 km, the rising air spreads

outward (c), which causes an overall

reduction in the surface air pressure. Over the adjacent water less warming takes place, so the air pressure is greater than that over land. The air

over the water moves toward the low-pressure area over the land, which sets up the daytime sea breeze. At night the land surface cools more rapidly than the water. The air over the land becomes dense and generates a land breeze.


Chapter 8 atmospheric circulation and pressure distributions

A valley breeze (a) forms when

daytime heating causes the

mountain surface to become

warmer than nearby air at the

same altitude. The air expands

upward and the air flows from

the valley to replace it. Nocturnal

cooling makes the air dense

over the mountain and initiates

a mountain breeze (b).


Chapter 8 atmospheric circulation and pressure distributions

El Niño is a recurrent event in the tropical eastern Pacific in which

sea-surface temperatures are significantly above normal.

La Niña is theinverse event (cold sea-surface temperatures).

The Walker circulation is an east-west circulation pattern of the Tropics, characterized by several cells of rising and sinking air connected by horizontal motions along parallel lines of latitude.

The Southern Oscillation is the reversal of surface pressure patterns over the tropical Pacific associated with El Niñoevents.

The Pacific Decadal Oscillation is an alternating pattern of sea surface temperature in the Pacific that reverses over several decades.


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