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7/30/2019 02 Wind Systems
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Global and LocalWind Systems
An Overview
Peter Busche
Deutsches Windenergie-Institut GmbH,DEWI Wilhelmshaven
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Main factors influencing wind systems
Explaining real wind systems using models
Global wind systems
Local wind systems
Wind Profile
Global and local wind systems
Contents:
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Winds: An Introduction
Classification TIME-DISTANCE SCALE EXAMPLES
Macroscale:1. Planetary2. Synoptic
Weeks to years (1000-40,000km)Days to weeks (100-5000km)
Westerlies & cyclonesanticyclones & hurricanes, jet streams
Mesoscale Minutes to days (1-100 km) Land-sea breezes, thunderstorms &
tornadoes
Microscale Seconds to minutes (< 1 km) Turbulence, dust devils and gustsTable 1.0: Scale of atmospheric wind systems. (adapted from Lutgens & Tarback, 1998)
Global wind systems- MacroscaleLocal wind systems - Mesoscale
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Winds: Driving Force
Wind mainly develop due to spatial atmospheric differencescaused by net solar radiation at different latitudes
Figure showing development of wind due to net solar radiation
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Reasons for the poleward flow at high altitudes
1. Convergence of hot air in the tropics (thermally driven)
2. Vertical Pressure Gradient
g = earth's acceleration, note:
= air density
R = gas constant
T = temperature
r = Earths radius
Standard Atmosphere: ISO 2533 -2 to 32 kmgeometrical- and geopotential altitude
= gdz
dp
TR
p
=
2
+=
hr
rgg n
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Main factors influencing wind systems
1. Pressure gradient force
p = the pressure difference between two points
= air density = 1.225 kg/m at standard conditions
d = distance (meters) between two points
2. Coriolis acceleration (force)
= angular rotation rate of the earth (7.27 E -5 1/s)u = geostrophic wind velocity
= the latitude (no Coriolis force at the Equator!,lattitude = 0)
3. Centripetal accelerationActs on air flowing around centres of circulation
4. Frictional decelerationActs in a direction opposite to the wind flow.
d
pPGF
=
1
Fc = 2**u*sinForce acting onmoving objectsdue to earths
rotation
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Coriolis forces- winds will be deflected to the right
in the northern hemisphere
- winds will be deflected to the left
in the southern hemisphere
- wind will rotate clockwise around
high pressure zone on northern hemisphere
- wind will rotate counter clockwise around
low pressure zone on northern hemisphere
- wind will rotate counter clockwise around
high pressure zone on southern hemisphere
- wind will rotate clockwise around
low pressure zone on southern hemisphere
as seen by an observer on the earth sitting
in the high pressure zone
NP
SP
EW
H
H
L earthrotation
L
H
L
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Geostrophic Winds / Surface Winds
Figure 1: Geostrophic wind Figure 2: Ageostrophic/real wind
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Explaining real wind systems using cell models
Single cell
model (Hadley) 3 cell model
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Global wind systems
(a) Imaginary uniform earth with idealised pressure belts and
(b) the real earth with zonal patterns disrupted by large landmasses,which cause semi-permanent high and low pressure cells.
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Actual weather map (The Westerlies)
Rossby Waves
Jet Streams
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
ITCZ (Intertropical convergence zone)
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Meteorology
Wind from sea
Thermals
Upwin
ds
Sea Beach Grass Trees Hills Woods Buildings Cities Valleys Mountains
Affecting the wind:
Temperature
Roughness
Obstacles
Orography
Sun = Source of Wind
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Local wind systems (1)
1. Land-Sea breeze
2. Anabatic-Katabatic winds
3. Mountain-Valley winds
4. Bora-Foehn
Local (Minor) wind systems are generally of interest only in
description of weather and local climate.However, the main ones occur quite often.
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Land breeze / Sea breeze
Sea breeze (daytime)
Land breeze (night)
(Thermally induced)
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Anabatic / Catabatic Wind
Anabatic winds
Catabatic winds
*Mountain-Valley windsare formed the same way
but are characterisedby flow along the valleys
(Thermally induced)
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Formed by deformation of air currents crossingmountain ranges
Fhn / Bora
(Orographically induced)
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Local wind systems (2)
Further (minor) local wind systems include:
1. Snow breeze
2. Cloud breeze
3. Land-river breeze
4. Local winds at urban heat islands
5. Eclipse winds
Deutsches Windenergie - Institut GmbH http://www.dewi.de
Wind systems in the Mediterranean Sea region
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Deutsches Windenergie - Institut GmbH http://www.dewi.de
Layers of the lower atmosphere
1000 m
100 m
5 mm laminal boundary layer
Surface layer
Prandtl layer
Ekman layer
free atmosphere
turbulent boundary layer
height
Deutsches Windenergie - Institut GmbH http://www.dewi.de
0
20
40
60
80
100
120
140
1980 1985 1990 1995 2000 2005 2010
Year
serial production
prototypes
Rotordiameter
,m
Development of size
600 kW
500 kW
300 kW
50 kW
2,500 kW
1,500 kW
4,500 kW
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0
10
20
30
40
50
60
70
80
90
100
0 1 2 3 4 5 6
Windspeed [m/s]
Height[m]
Water
Grass
City
Geostrophic Wind1000
BoundaryLayer
SurfaceLayer
Geostrophic windinduced by large-scalepressure distribution
Wind speed increasingwith height
Inside the surface layer:logarithmic wind profile
Vertical wind profile
Deutsches Windenergie - Institut GmbH http://www.dewi.de