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Weather 101 and beyond

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Title: ATM OCN 100 Summer 1999 Subject: 3. AIR TEMPERATURE Author: Edward J. Hopkins Last modified by: Classroom Computing Created Date: 5/26/1998 8:52:52 PM – PowerPoint PPT presentation

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Title: Weather 101 and beyond


1
Weather 101 and beyond
  • Edward J. Hopkins
  • Dept. of Atmospheric Oceanic Sciences
  • Univ. of Wisconsin-Madison
  • Midwest Hot Air Balloon Safety Seminar
  • Hot Aireventure
  • Oshkosh 3 March 2001

2
Concerns of Balloonists
  • The Weather
  • The Terrain (or Surface)

3
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4
Quiz
  • Ballooning (Fair) Weather is associated with High
    or Low Pressure?
  • Which way do winds blow around High pressure?
  • Low pressure?

5
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6
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7
WIND
  • What is Wind?
  • Why the wind?
  • Review of basic concepts

8
ASOS Wind InstrumentsWind Vane (left) Cup
Anemometer (right)
9
Aerovane Measures wind speed direction
10
BEAUFORT WIND FORCE SCALEModern version,
Source Federal Meteorological Handbook I
11
BEAUFORT WIND FORCE SCALE (cont.)
12
The wind responds to a Difference in air pressure
13
BASIC CONCEPTS Air Pressure (cont.)
14
Explaining Differences in Air Pressure
  • Low Pressure
  • High Pressure

15
Display of Pressure Differences on a Weather Map
- Isobars
16
Isobars -- lines of equal barometric pressure-
use sea level corrected pressure
17
AIR PRESSURE in the Vertical (cont.)
18
As a Sidebar Altimetry
  • Since pressure decreases at a reasonably known
    rate of 1 mb decrease per 10 meter rise or
    0.01 inch of Hg per 10 feet,
  • then pressure altimeters are barometers made to
    read in altitude.
  • But...

19
Pressure Change with height depends upon
Temperature of column - (It is really the
density!)
20
WHY THE WIND? (cont.)
  • Reasons for Atmospheric Motions
  • Buoyancy Effects or Dynamic Effects

21
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22
Daily Heating
Heat Gain
Heat Loss
Daylight
Nighttime
23
January Temperatures - Madison, WI (1981-90)
Daylight
Nighttime
Nighttime
24
January Wind Speeds - Madison, WI (1981-90)
Nighttime
Daylight
Nighttime
25
July Temperatures - Madison, WI (1981-90)
Daylight
Nighttime
Nighttime
26
July Wind Speeds - Madison, WI (1981-90)
Daylight
Nighttime
Nighttime
27
ENERGY TRANSPORT CONVECTION
28
LAPSE CONDITIONSTemperature decreases with height
29
ISOTHERMAL CONDITIONS Temperature remains
constant with height
30
INVERSION CONDITIONS Temperature increases with
height
31
U.S. STANDARD ATMOSPHERE See Fig. 1.9 Moran
Morgan (1997)
Thermosphere
Mesopause
Mesosphere
Stratopause
Stratosphere
Tropopause
Troposphere
32
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33
WHY THE WIND? (cont.)
  • Reasons for Atmospheric Motions
  • Buoyancy Effects or Dynamic Effects

34
Air Converging Aloft
35
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36
Air Diverging Aloft
37
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38
The Surface
  • The Obvious
  • Obstacles to take-off and landing (e.g., trees,
    power lines, animals)
  • The Surface and the Winds
  • Affects the Boundary Layer wind flow
  • Can produce local wind regimes

39
Boundary Layer
  • Where we live
  • Extends from surface to approximately 3000 ft.
    (1000 m)
  • Consists of
  • Surface Boundary Layer (30 to 60 ft. includes
    Anemometer Level)
  • Ekman or Spiral Layer (above 60 ft. to Free
    Atmosphere)

40
Relative Surface RoughnessSource Stull, 1995
41
B. EXPLANATIONS of ATMOSPHERIC MOTION
  • Practical Problems
  • Historical Concepts
  • Forces of Motion Newton's Laws

42
An example of an equation of motionNASA
43
PRESSURE GRADIENT FORCE
44
PRESSURE GRADIENT FORCE (cont.)
45
ASSUMPTIONS
  • For convenience, assume that
  • Winds are nearly horizontal
  • Atmosphere is in nearly hydrostatic balance
    i.e., air parcels do not accelerate
    upward or downward

46
HYDROSTATIC BALANCE CONCEPT See Fig. 9.11 Moran
Morgan (1997)
47
HORIZONTAL PRESSURE GRADIENT FORCE
(cont.)Direction is from High to Low pressure!
48
HORIZONTAL PRESSURE GRADIENT FORCE (cont.) See
Fig. 9.1 Moran Morgan (1997) Magnitude depends
on isobar spacing!
49
LOCAL WINDSFLOW RESPONDING TO PRESSURE GRADIENT
FORCE - LOCAL WINDS
  • Assumptions
  • Only Pressure gradient force operates
  • Results from temperature differences
  • Acts for short time short distances.
  • Examples
  • Sea-Land Breeze Circulation
  • Mountain-Valley Breeze Circulation
  • City-Country Circulation

50
Sea (Lake) Breeze(Graphics from UIUC WW2010)
51
VERTICAL PRESSURE GRADIENTS - Dependency on
density (temperature)
52
Sea (Lake) Breeze (cont.)
53
Sea (Lake) Breeze (cont.)
54
Sea (Lake) Breeze (cont.)
55
Sea (Lake) Breeze (cont.)
56
Sea (Lake) Breeze (cont.)
57
Sea (Lake) Breeze (cont.)
(Lake)
58
Sea (Lake) Breeze (cont.) See Fig. 12.2 A Moran
Morgan (1997)
59
Land Breeze
60
Land Breeze (cont.)
61
Land Breeze (cont.)
62
Land Breeze (cont.) See Fig. 12.2 B Moran
Morgan (1997)
63
Mountain Breeze See Fig. 12.14 Moran Morgan
(1997)
64
Valley BreezeSee Fig. 12.14 Moran Morgan
(1997)
65
Larger Scale Flow
  • Observation

66
Right with Height
67
PRESSURE GRADIENT FORCE
68
Reason for the Problem Because the earth turns
69
CORIOLIS EFFECT or FORCE (cont.)
70
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71
Geostrophic Adjustment
72
Geostrophic Wind See Fig. 9.12 Moran Morgan
(1997)
73
Flow in Friction Layer
74
Variation of Friction Effects with Height
75
Right with Height
76
Varying effects of Surface Roughness
77
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78
Curved Flow
79
Features in a Surface Low (Convergence Ascent)
80
Features in a Surface High (Sinking Divergence)
81
Numerical Weather Prediction
82
Numerical Weather Prediction
83
Numerical Weather Prediction
84
My office Dept. of Atmospheric Oceanic
Sciences hopkins_at_meteor.wisc.edu
85
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86
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87
UNSTABLE CONDITIONS Compare Environment with
DALRWarmer parcel continues upward
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