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Next Week: QUIZ One question from each of week: –9 normal lectures + global warming lecture –Over main topic of lecture and homework Multiple choice,

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Presentation on theme: "Next Week: QUIZ One question from each of week: –9 normal lectures + global warming lecture –Over main topic of lecture and homework Multiple choice,"— Presentation transcript:

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2 Next Week: QUIZ One question from each of week: –9 normal lectures + global warming lecture –Over main topic of lecture and homework Multiple choice, short answer, matching, map question Powerpoints: http://www.aos.wisc.edu/~ahulme/aos101/

3 AOS 101 April 15/17 Thickness and Thermal Wind

4 Thickness The vertical distance in meters between two pressure levels 1000 hPa = 0 m 500 hPa = 5600 m THICKNESS = 5600 m – 0 m = 5600 m Z

5 Consider a column… Cool the average temperature of the column by 20 K Air becomes more dense, mass stays the same so volume must decrease Air takes up less space COLUMN SHRINKS 1000 hPa = 0 m 500 hPa = 5600 m COOL

6 Consider a column… Cool the average temperature of the column by 20 K Air becomes more dense, mass stays the same so volume must decrease Air takes up less space COLUMN SHRINKS 1000 hPa = 0 m 500 hPa = 5000 m COOL Z = 5000 m

7 Consider a column… Warm the average temperature of the column by 20 K Air becomes less dense, mass stays the same so volume must increase Air takes up more space COLUMN EXPANDS 1000 hPa = 0 m 500 hPa = 5600 m WARM

8 Consider a column… Warm the average temperature of the column by 20 K Air becomes less dense, mass stays the same so volume must increase Air takes up more space COLUMN EXPANDS 1000 hPa = 0 m 500 hPa = 6200 m WARM Z = 6200 m

9 Summary COOL air will result in LOW THICKNESS WARM air will result in HIGH THICKNESS Thus, the thickness between two pressure layers is proportional to the average temperature of that layer Z ≈ const x T ave

10 Thermal Wind Not an actual wind “Blows” along thickness contours with cold (low thickness) air to the left Stronger temperature gradients imply stronger thermal wind Equal to the SHEAR of the wind (i.e. is related to the observed wind)

11 V 850 V 200 VTVT

12 VTVT 5660 m COLD WARM 5600 m 5540 m

13 Clockwise turning of winds with height VeeringBacking 850 hPa 300 hPa 850 hPa 300 hPa VTVT VTVT Counterclockwise turning of winds with height WARM AIR ADVECTIONCOLD AIR ADVECTION

14 Midlatitude Weather Upper-level winds will be much stronger than low-level winds –i.e. thermal wind will be very close to upper- level wind Consider a front with cold air to the north and warm air to the south.

15 COOLWARM P = 500 hPa Geostrophic wind into page Thermal wind into page LOW heightsHIGH heights NORTH PGF P = 700 hPa

16 Thermal Wind Balance Pressure gradient increases with height –Winds increase with height Thus, areas of strong temperature (thickness) gradient will have strong winds above them.

17 700 hPa Temperature 500-850 hPa Thickness

18 500 hPa Height 500 hPa Wind Speed

19 500-850 hPa Thickness 500 hPa Wind Speed

20 Cyclone Symbols: Point in direction of front movement COLD WARM OCCLUDED STATIONARY

21 Warm Front COOL WARM

22 Associated Weather (WF) Gradual Slope Stratiform rain –long lasting light rain –occurs on cool side of front Temperature increases prior to frontal passage Wind becomes southerly after passage

23 Cold Front COOL WARM

24 Associated Weather (CF) Much Steeper Slope More intense (convective) rain –Thunderstorms for a shorter period –occurs on warm side of front Temperature decreases after frontal passage Wind becomes northerly after passage

25 L LIGHTER RAIN HEAVIER RAIN WARM AIR COLD AIR COOL AIR

26 Finding a Front Temperature (dewpoint) Gradient Change in wind direction –Converging winds at the front “Kink” or “trough” in isobars (lower pressure) Banded precipitation

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28 Upper-level terminology TROUGH: area of lower heights RIDGE: area of higher heights L H


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