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Local Wind Systems and Temperature Structure in Mountainous Terrain. Met 130 6 May 2008 Dr. Craig Clements. Types of Thermally-Driven Winds found in Mountainous Regions. 1. Plain-Mountain Winds 2. Valley Winds 3. Slope Winds. Thermally-driven refers to the forcing - PowerPoint PPT Presentation
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Local Wind Systems and Temperature Structure in Mountainous Terrain
Met 1306 May 2008
Dr. Craig Clements
Types of Thermally-Driven WindsTypes of Thermally-Driven Windsfound in Mountainous Regionsfound in Mountainous Regions
1. Plain-Mountain Winds1. Plain-Mountain Winds
2. Valley Winds2. Valley Winds
3. Slope Winds3. Slope Winds
Thermally-driven refers to the forcing Thermally-driven refers to the forcing due to temperature differences!due to temperature differences!
Thermally-Driven Winds Found in Mountains
Whiteman(2000)
Cross-section of a Mountain Valley
Whiteman(2000)
Daytime:
Air is warmer in the valley than over the plain
Pressure is lower in the valley and higher over the plain at the same elevation
The pressure gradient force is directed from the plain to the valley
A up-valley wind is produced that blows from the plain into the valley.
Nighttime:
Pressure gradient force reverses direction
A down-valley wind occurs
Down-Valley Winds
Valley Winds
Up-Valley Winds
Whiteman(2000)
Up-Valley and Down-Valley Surface Winds(Measured in Yosemite National Park)
Date and Time
A SODAR (sound-detection-ranging) is similar to RADAR
Yosemite National Park, 12 Aug. 2003
Vertical Structure of Down-Valley Winds
‘Nose’ of Down-valley
wind
Nose is location of Wind speed
maximum
Conceptual wind models for mountain valleys
(Whiteman 1982)
The Volume Effect of Valleys
Whiteman(2000)
Examples of Valley Shapes
Whiteman(2000)
Yosemite Valley, Yosemite National Park
Inversion destructionModels in mountain Valleys (Whiteman 1982):
Pattern 1
Inversion destructionModels in mountain Valleys (Whiteman 1982):
Pattern 2
Inversion destructionModel in mountain Valleys (Whiteman 1982):
Pattern 3
Diurnal Temperature Evolution in Mountain Valleys
(from Stull 1988; adapted from Whiteman 1982)
dzudzR
cTdzudz
t p
)()ˆ(
A Simplified Heat Budget of the Valley Atmosphere
Term 1: local rate of change of potential temperatureTerm 2: convergence of potential temperature flux by mean windTerm 3: convergence of radiative fluxTerm 4: convergence of turbulent sensible heat flux
Mass conservation in a valley
valley
plain
xy
valley
xy
plain
A h
V
A h
V
Topographic Amplification Factor (TAF)
)(tSAhcTdt
dhfo
p
The thermodynamic model developed by Whiteman and McKee (1982):
21
12 1cos2
io
pi ttAA
cThh
Heig
ht (m
AGL
)
0
100
200
300
400
500
600
700
282 284 286 288 290 292 294 296 298
600 PST
630
700
725
955
1035
2 3 4 5 6 7 8 -6 -4 -2 0 2 4 6
Up-valley Wind Component (m s-1)Mixing Ratio(g kg-1)Potential Temperature (K)
Tethersonde Profiles from Yosemite Valley
0
100
200
300
400
500
600
700
800
0 1 2 3 4 5 6 7 8 9 10 11Time after sunrise (Hour)
1.46
1.78
1.86
2.25
6.31
7.43
0
100
200
300
400
500
600
700
800
0 0.5 1 1.5 2 2.5 3 3.5 4Time after sunrise (hour)
1.46
1.78
1.86
2.25
6.31
7.43
Inversion breakup according to Eq. 2 with Ao = 0.45, (a) = 0.007 K m-1 and (b) = 0.015 K m-1 TAF () values are indicated in legend.
(a)
(b)
Modeled Inversion destruction
• Slopes winds are usually in the range of 1-4 m/s (2-8 mph); are weaker and more gentle than valley winds.• Peak wind speed occurs a few meters above the the slope surface.• Daytime upslope winds are typically stronger and deeper than nighttime downslope winds. • A transition period occurs between the upslope and downslope winds in evening and morning. (See Time-Lapse Video)
Slope winds
Whiteman(2000)
Consequences of downslope flows: movie
Downslope winds can produce a cold air pool in a valley or basin. Some of these cold air pools can last several days to a week, trapping pollutants in the valley/basin. Cold air pools are often associated with dense fog, which is hazardous to aviation.
Whiteman(2000)
Downslope winds are often called drainage winds
Glacier WindsA cold air layer forms over ice surface and flows downhill.
Whiteman(2000)
Diurnal Evolution of the Boundary Layer over Mountains
Whiteman(2000)
The layer of air influenced by the earth’s surface is called the planetary boundary layer (PBL).