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Atmospheric and Oceanic Circulations (continued) Chapter 6

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Atmospheric and Oceanic Circulations (continued) Chapter 6. Lecture 14 4 February 2005. Figure Credit: “Earth’s Climate” by W. Ruddiman. Figure Credit: “Earth’s Climate” by W. Ruddiman. Credit: www.physicalgeography.net. Wind. - PowerPoint PPT Presentation
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Lecture 14 4 February 2005 Atmospheric and Oceanic Circulations (continued) Chapter 6
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Page 1: Atmospheric and Oceanic Circulations (continued) Chapter 6

Lecture 144 February 2005

Atmospheric and Oceanic Circulations(continued)

Chapter 6

Page 2: Atmospheric and Oceanic Circulations (continued) Chapter 6

Figure Credit: “Earth’s Climate” by W.

Ruddiman

Page 3: Atmospheric and Oceanic Circulations (continued) Chapter 6

Figure Credit: “Earth’s Climate” by W. Ruddiman

Page 4: Atmospheric and Oceanic Circulations (continued) Chapter 6

Credit: www.physicalgeography.net

Wind simply put, wind is the horizontal flow of air

in response to differences in air pressurethese pressure differences are usually

due to uneven solar heating at the surface

wind flows because of

pressure gradient

‘heat rises’

Page 5: Atmospheric and Oceanic Circulations (continued) Chapter 6

Wind

winds are designated as direction fromnot direction to

(oceanographers do it the opposite)

wind compass

so, a westerly wind would be coming from what angular

direction?

Page 6: Atmospheric and Oceanic Circulations (continued) Chapter 6

Four forces that determine winds

1. Gravity - pulls gas molecules close to Earth density & pressure decrease with height

2. Pressure gradient force - the difference in air pressure between

areas3. Coriolis force - deflects wind from a

straight line to the right or left depending on hemisphere

4. Friction force - the drag on air flow from the Earth’s surface

Page 7: Atmospheric and Oceanic Circulations (continued) Chapter 6

Pressure vs. Pressure Gradient

•The value of pressure itself is NOT

important

•The CHANGE in pressure over DISTANCE

is

•Change over distance is a GRADIENT

•The GRADIENT in pressure gives winds &

ocean currents their “push”

Page 8: Atmospheric and Oceanic Circulations (continued) Chapter 6

Pressure Gradient Force (PGF)

isobar - a line of equal pressure (analogous to

isotherm)

gradient is 16 mb(note the closer isobars)

the PGF acts at right (90º) angles to the isobars

Page 9: Atmospheric and Oceanic Circulations (continued) Chapter 6

Pressure Gradient Force

note the 1008 mb isobar

Page 10: Atmospheric and Oceanic Circulations (continued) Chapter 6

Wind speed = Const * Pressure Gradient

Here, a 4x increase in PGF corresponds to a 4x increase in wind speed

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Page 11: Atmospheric and Oceanic Circulations (continued) Chapter 6

Pressure Gradient Force and Isobars

if there were no other forces acting on wind, it would flow in straight lines (perpendicular to isobars) from high to low pressure zones

Page 12: Atmospheric and Oceanic Circulations (continued) Chapter 6

Coriolis Force (just the facts)

• Rotation of Earth acts to deflect any motion

from a straight line

• Deflection is to right (NH) to the left (SH)

• Coriolis “force” act on a right angle to the

motion

• Coriolis Force is NOT a real “force” but is

caused by viewing motion on a rotating

planet

Page 13: Atmospheric and Oceanic Circulations (continued) Chapter 6

Coriolis Force

• Show the merry-go-round video

Page 14: Atmospheric and Oceanic Circulations (continued) Chapter 6

the amount of rotation about a vertical axis

(’spinning’) is maximum at the poles and minimum at

the equator

Figure Credit: “Earth’s Climate” by W.

Ruddiman

Page 15: Atmospheric and Oceanic Circulations (continued) Chapter 6

Earth’s Rotationevery point on earth rotates around a central

axis at 15 degrees/hour

LatitudeSpeed of

rotation (mph)0˚ 1041

30˚ 902

50˚ 670

60˚ 521

90˚ 0

Page 16: Atmospheric and Oceanic Circulations (continued) Chapter 6

Coriolis Forcean object with an initial east-west velocity will maintain that velocity,

even as it passes over

surfaces with different velocities

as a result, it appears to be deflected over that surface (right in NH, left in SH)

Page 17: Atmospheric and Oceanic Circulations (continued) Chapter 6

Coriolis Force and Deflection of Flight Path

Page 18: Atmospheric and Oceanic Circulations (continued) Chapter 6

Coriolis Force and Deflection of Flight Path

Page 19: Atmospheric and Oceanic Circulations (continued) Chapter 6

Coriolis Force and Flight Paths II.

Airplane animation

Page 20: Atmospheric and Oceanic Circulations (continued) Chapter 6

Figure Credit: “Earth’s Climate” by W.

Ruddiman

The Coriolis Force affects air flow in response to pressure gradients in the

atmosphere

Page 21: Atmospheric and Oceanic Circulations (continued) Chapter 6

geostrophic winds - PGF and Coriolis forces are opposite and balanced

Credit: www.physicalgeography.net

in the northern hemisphere (upper troposphere), the CF deflects the wind to

the right until wind flows parallel to isobars

~7km

Page 22: Atmospheric and Oceanic Circulations (continued) Chapter 6

Geostrophic Winds

Balance between Pressure Gradient & Coriolis

Forces

Flow along isobars not across

Works for upper atmosphere winds & ocean

currents

Page 23: Atmospheric and Oceanic Circulations (continued) Chapter 6

500 mb Pressure Map

Page 24: Atmospheric and Oceanic Circulations (continued) Chapter 6

PGF, CF & isobars in upper troposphereisobars

Page 25: Atmospheric and Oceanic Circulations (continued) Chapter 6

Friction Force

surface friction reduces wind speed and reduces the Coriolis force (remember CF

increases with wind speed)because of this, it causes winds to

move across isobars at an angle

the friction force operates only in the bottom 0.5-1 km of the atmosphere,

and it acts opposite to the direction of motion

Page 26: Atmospheric and Oceanic Circulations (continued) Chapter 6

Figure Credit: “Earth’s Climate” by W.

Ruddiman

Page 27: Atmospheric and Oceanic Circulations (continued) Chapter 6

PGF + Coriolis + Friction Forces

isobars

Page 28: Atmospheric and Oceanic Circulations (continued) Chapter 6
Page 29: Atmospheric and Oceanic Circulations (continued) Chapter 6

The inter-tropical convergence zone (ITCZ)solar heating in the tropics expands air and

decreases its density - leading to increased buoyancy

How would this change the average molecular weight of air?

average molecular weight of air is ~29

g/mol

average density of air is 1.3 kg/m^3

what happens to air density if

you add water vapor?

It also gets more humid (adding water vapor)

Page 30: Atmospheric and Oceanic Circulations (continued) Chapter 6

Convection on your Stove

Page 31: Atmospheric and Oceanic Circulations (continued) Chapter 6

Convection on Earth

Page 32: Atmospheric and Oceanic Circulations (continued) Chapter 6

as this air rises, it cools and water condenses out, leading to intense

precipitation

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Page 33: Atmospheric and Oceanic Circulations (continued) Chapter 6

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A satellite (GOES) view of the ITCZ over the eastern Pacific

Page 34: Atmospheric and Oceanic Circulations (continued) Chapter 6

the position of the ITCZ tracks the sun (it is found in the summer hemisphere) - the

location of the ITCZ determines the rainy season in many tropical countries, especially

those in Africa

the horizontal winds within the ITCZ are calm - the doldrums

Page 35: Atmospheric and Oceanic Circulations (continued) Chapter 6

The C in ITCZ

the intense uplift of air creates horizontal pressure gradients at the surface

Credit: NASA JPL

as a result, winds converge towards the equator from both hemispheres

what about the complete cycle - where does the uplifted air go?

Page 36: Atmospheric and Oceanic Circulations (continued) Chapter 6
Page 37: Atmospheric and Oceanic Circulations (continued) Chapter 6

Equator-to-pole cross section of circulation

Page 38: Atmospheric and Oceanic Circulations (continued) Chapter 6

Hadley cell circulation

this circulation refers to the complete circulation of rising air in the tropics,

descending air over 30 °N and °S, and trade winds converging at the equator

the descending branch of the Hadley circulation brings hot, dry air to the surface -

leading to high pressure areas and suppressed precipitation

Page 39: Atmospheric and Oceanic Circulations (continued) Chapter 6

Subtropical high-pressure cellsthese cells occur where the tropical air

descends in either hemisphere

Page 40: Atmospheric and Oceanic Circulations (continued) Chapter 6

Figure

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Page 41: Atmospheric and Oceanic Circulations (continued) Chapter 6

Figure

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Page 42: Atmospheric and Oceanic Circulations (continued) Chapter 6

Figure Credit: physicalgeography.net

Monsoon Circulation

Page 43: Atmospheric and Oceanic Circulations (continued) Chapter 6

Asian monsoo

nintense, dry winds flow from the Asian interior in response

to the gradient between the

continental high pressure and the equatorial (ITCZ)

low pressure

Page 44: Atmospheric and Oceanic Circulations (continued) Chapter 6

Asian monsoo

nin summer, the subsolar point

and the ITCZ shift northward,

reversing the pressure gradient

- as the winds flow over the

Indian ocean they gain moisture

Page 45: Atmospheric and Oceanic Circulations (continued) Chapter 6

Daytime land-sea breeze

results from differential heating of land and sea - not from radiation differences - but

from the different specific heats of land and water

Page 46: Atmospheric and Oceanic Circulations (continued) Chapter 6

Nighttime land-sea breeze

at night, the land cools more rapidly than the sea and thus overlying air becomes more

dense and has a higher pressure


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