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MADISON’S CURRENT WEATHER
Madison Weather at AM CDT 31 JUL 2002 Updated twice an hour at :05 and :25 Sky/Weather: MOSUNNY Temperature: 83 F (28 C) Dew Point: 66 F (18 C) Relative Humidity: 56% Wind: SW8 MPH Barometer: 30.00S ( mb)
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Last 24 hrs in Madison FOG
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CURRENT VISIBLE
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Current Surface Weather Map with Isobars (“iso” = equal & “bar” = weight), Fronts and Radar
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Current Temperatures (°F) & Isotherms (“iso” = equal +”therm” = temperature)
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Current Dewpoints (oF)
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Tomorrow AM Forecast Map
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Current Surface Weather Map with Isobars (“iso” = equal & “bar” = weight), Fronts and Radar
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H L L L L H L H L L H H L H L L L L H H H H
Current Surface Winds with Streamlines & Isotachs (“iso” = equal & “tach” = speed) H L L L L H L H L L H H L H L L L L H H H H
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Current 5,000 ft. Winds with Streamlines & Isotachs (“iso” = equal & “tach” = speed)
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Current 10,000 ft. Winds with Streamlines & Isotachs (“iso” = equal & “tach” = speed)
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Current 34,000 ft. Winds & Jet Stream with Streamlines & Isotachs (“iso” = equal & “tach” = speed)
Trough Ridge
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ATM OCN 100 - Spring 2002 LECTURE 20 (con’t.)
THE THEORY OF WINDS: PART III - RESULTANT ATMOSPHERIC MOTIONS (con’t.) Introduction & Assumptions Buys-Ballot Law Hydrostatic Balance Relationship Horizontal Equation of Motion Local Winds Geostrophic Winds Winds in Friction Layer
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Summary of Forces for selected models See Table 9
Summary of Forces for selected models See Table 9.1 Moran & Morgan (1997) MODELS
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Current Midwest Weather Plot
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L H Current Midwest Weather Analysis
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Flow in Friction Layer See Fig. 9.15 Moran & Morgan (1997)
No Friction Geostrophic Friction Subgeostrophic
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Flow in Friction Layer See Fig. 9.15 Moran & Morgan (1997)
Vector Magnitude 1. Depends on Friction 2. Less than Geostrophic Wind Vector Direction: Angles across isobars Toward Low in either hemisphere
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Observation: Right with Height
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Variation of Friction Effects with Height See Fig. 9
Variation of Friction Effects with Height See Fig Moran & Morgan (1997)
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Varying effects of Surface Roughness
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Variations in Surface Roughness leads to divergence/convergence patterns See Fig Moran & Morgan (1997)
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F. CURVED, HORIZONTAL BALANCED MOTION - “GRADIENT FLOW”
Assumptions Without Friction Two Cases
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Summary of Forces for selected models See Table 9
Summary of Forces for selected models See Table 9.1 Moran & Morgan (1997)
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“GRADIENT” FLOW: ANTICYCLONIC Case See Fig. 9
“GRADIENT” FLOW: ANTICYCLONIC Case See Fig Moran and Morgan (1997):
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“GRADIENT” FLOW: ANTICYCLONIC Case See Fig. 9
“GRADIENT” FLOW: ANTICYCLONIC Case See Fig Moran and Morgan (1997):
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“GRADIENT” FLOW: CYCLONIC Case See Fig. 9.14 Moran and Morgan (1997):
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“GRADIENT” FLOW: CYCLONIC Case See Fig. 9.14 Moran and Morgan (1997):
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G. GRADIENT FLOW WITH FRICTION
Resultant flow with Friction FCentripetal = FPG,H + FCor + FFriction (A vector summation).
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Summary of Forces for selected models See Table 9
Summary of Forces for selected models See Table 9.1 Moran & Morgan (1997)
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G. GRADIENT FLOW WITH FRICTION
Resultant flow with Friction FCentripetal = FPG,H + FCor + FFriction (A vector summation). Applicability to the Atmosphere Situation Resultant Diagrams
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Anticyclonic Flow in Friction Layer
Fig Moran & Morgan (1997)
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Cyclonic Flow in Friction Layer
Fig Moran & Morgan (1997)
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Near-Surface Winds in each Hemisphere See Figs. 9. 17 & 9
Near-Surface Winds in each Hemisphere See Figs & 9.18 Moran & Morgan (1997)
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Summary of Forces for selected models See Table 9
Summary of Forces for selected models See Table 9.1 Moran & Morgan (1997)
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H. RELATIONSHIPS BETWEEN HORIZONTAL & VERTICAL MOTIONS
Dilemma Convergence / Divergence Principle of Mass Continuity
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Features in a Surface Low (Convergence & Ascent)
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Features in a Surface High (Sinking & Divergence)
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H. RELATIONSHIPS BETWEEN HORIZONTAL & VERTICAL MOTIONS (con’t.)
Dines’ Compensation Resultant Vertical Motions Implications of Dines' Compensation
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I. VORTICES & VORTICITY Definitions Characteristic Vortex Features
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Anticyclonic Vorticity
Types of Vorticity Cyclonic Vorticity Anticyclonic Vorticity
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Vorticity Conservation of Vorticity
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ATM OCN 100 - Summer 2002 LECTURE 24 PLANETARY-SCALE CIRCULATION of EARTH'S ATMOSPHERE
A. INTRODUCTION Why do weather systems in mid latitudes move from west to east? but.. tropics move from east to west?
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Typical Movement of Storms
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Year 2001 Hurricane/Tropical Storm Tracks in North Atlantic
8 Hurricanes 7 Trop. Storms
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Year 2001 Hurricane/Tropical Storm Tracks in Eastern/Central North Pacific
8 Hurricanes 7 Trop. Storms
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B. GLOBAL SCALE PREVAILING SURFACE WINDS
Historical Wind Observations Popular Names of Principal Prevailing Surface Wind Regimes Where…
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Popular Names of Global-Scale Prevailing Wind Belts
Polar easterlies Westerlies Horse Latitudes NE Trades Doldrums SE Trades Horse Latitudes Westerlies Polar easterlies
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Average Air Pressure & Atmospheric Circulation
Polar Highs (or anticyclones) Subpolar Lows (or cyclones) Subtropical High Pressure Cells Intertropical Convergence Zone (ITCZ) ~ Subtropical High Pressure Cells Subpolar Lows (or cyclones
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Relationships between Prevailing winds & Major Pressure Patterns
C. AVERAGE SEA-LEVEL PRESSURE PATTERNS See Table 10.1 Moran & Morgan (1997) Relationships between Prevailing winds & Major Pressure Patterns
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Planetary Scale Circulation Regime See Figure 10
Planetary Scale Circulation Regime See Figure 10.4, Moran & Morgan (1997)
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PRESSURE PATTERNS (con’t.)
Relationships between winds, “centers of action” & oceanic circulation.
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OCEAN CURRENTS
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Gulf Stream
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Current Sea Surface Temperature
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Sea Surface Temperature – Late Fall
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PRESSURE PATTERNS (con’t.)
Relationships between “centers of action”, clouds & precipitation.
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Current Satellite Composite
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December Satellite Composite
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Average Cloudiness -- Annual
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Annual Percent Possible Sunshine
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ANNUAL AVERAGE CONTINENTAL PRECIPITATION
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PRESSURE PATTERNS (con’t.)
Relationships between “Centers of Action” & Major Biome Patterns Tropical Rain Forests Subtropical Deserts Mid latitude Biomes Polar Deserts
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LANDCOVER (VEGETATION DISTRIBUTION) Oak Ridge National Laboratory
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Global Biosphere From NASA (Goddard Space Flight Center)
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Köppen Climate Classification Scheme See Fig. 18
Köppen Climate Classification Scheme See Fig Moran & Morgan (1997)
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D. PLANETARY SCALE CIRCULATION: THEORETICAL ASPECTS
Historical Perspective George Hadley in 1730’s William Ferrel in 1850’s
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Simple Thermal Circulation Cells
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Simple Thermal Circulation on a non-rotating earth See Fig. 10
Simple Thermal Circulation on a non-rotating earth See Fig A Moran & Morgan (1997)
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HADLEY’S MODEL See Fig. 10.1 A&B Moran & Morgan (1997)
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More Recent Model of Planetary Atmospheric Circulation on a Rotating Earth See Fig C&D Moran & Morgan (1997)
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See Fig. 10.1 C&D Moran & Morgan (1997)
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Cross Sections through the Tropical Hadley Circulation Cells Fig. 10
Cross Sections through the Tropical Hadley Circulation Cells Fig Moran & Morgan (1997)
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North-South View of Planetary Scale Circulation Figure 10
North-South View of Planetary Scale Circulation Figure 10.7 Moran & Morgan (1997)
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D. PLANETARY SCALE CIRCULATION: THEORETICAL ASPECTS (con’t.)
Overall Observed Vertical Wind Structure Discovery of the Jet Stream
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Average 300 mb jet stream winds - Jan
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