Survey
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Chapter 11 Atmospheric Circulation: Local & Global Wind Systems General Circulation – the average flow of the atmosphere across the entire planet over long periods of time. Q: Why do we have global circulations? A.:Unequal heating of the earth’s surface. Tropics net gain Poles net loss To achieve balance between these regions, heat is transported from Tropics to poles. The first person to attempt a description of this redistribution: George Hadley – 1700’s Hadley Cell H equator L L L One-cell model of the atmosphere Original Hadley Cell – entirely convective (like a thunderstorm) This would actually occur if we assume: 1. Uniform water surface (no land-water discontinuities) 2. Sun is always over equator 3. Earth does not rotate. Thermally direct circulation = warm air moves up and cold, down Thermally indirect circulation = warm moves down and cold, up 60 30 Eq 30 60 3 – Cell Model 1. Still uniform water surface 2. Still sun always over equator BUT 3. ALLOW IT TO ROTATE Quite similar to actual earth circulation process: 1. Ascent in ITCZ 2. Turn poleward at tropics 3. Cool by radiation 4. Sink at ~30N (subtropical high) 5. Split poleward and equatorward (subtropical high) 6. Sink at poles, turn equatorward. 7. Converge with southerly flow to south (polar front low) Real World: 1. Land – Water contrasts 2. “Moving” sun across face of planet as well as rotation Pressure Patterns: January (North Hemisphere) Bermuda - Azores High and Pacific High (25-35N) Icelandic Low and Aleution Low (40-65N) Siberian High ITCZ farther south July (North Hemisphere) Bermuda High and Pacific High are stronger Icelandic Low is weaker and Aleution Low is GONE Siberian High is gone ITCZ is farther north Precipitation Patterns ITCZ Average Wind Flow Variance of speeds greater in NH SH mostly water Slower to warm and cool Stronger winds in the winter hemisphere Jet Streams A switfly flowing current of air thousands of kilometers long, a few hundred kilometers wide, and 1-2 kilometers deep. Usually at 10-15 km altitude. Subtropical Jet Stream - ~13 km Polar Front Jet Stream - ~ 10km Jet Streak – a region of locally strong wind speeds. Formation of Jet Streams 1. Polar Front Jet Sharp change in temperature across polar front jet Sharp change in pressure across polar front jet (height of pressure surface) Strong pressure / height gradient intensifies wind speed 2. Subtropical Jet Stream There is some evidence of a “subtropical front” aloft due to heat transport by Hadley Cell Governed somewhat by angular momentum Objects in motion possess MOMENTUM Linear Momentum massobject * velocityobject Angular Momentum Mass*velocity*radiual distance from axis At the equator, the Earth rotates eastward at > 1,000 mph On a calm day at the equator, air above the surface also moves eastward at > 1,000 mph Since parcels in motion are on the rotating planet earth, they possess ANGULAR MOMENTUM. If there are no net external twisting forces acting on a rotating system, then the angular momentum of the system does not change. Ice Skater Arms extended slow rotation Arms tucked-in fast rotation rs > rn for m=constant: r decreases, v increases r increases, v decreases 1. 2. 3. 4. 5. Parcels rise at equator Parcels turn poleward r decreases v increases at turn to the right Generates westerlies aloft