wind science 101: i. overview of wind patterns

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Wind Science 101: I. Overview of Wind Patterns. Eugene S. Takle Professor Department of Agronomy Department of Geological and Atmospheric Science Director, Climate Science Program Iowa State University Ames, IA 50011. WESEP REU Short Course Iowa State University Spring 2011. Outline. - PowerPoint PPT Presentation

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Wind Science 101:I. Overview of Wind Patterns

Eugene S. TakleProfessor

Department of AgronomyDepartment of Geological and Atmospheric Science

Director, Climate Science ProgramIowa State University

Ames, IA 50011

WESEP REU Short CourseIowa State University

Spring 2011

Outline Global scale 3-D global circulation patterns and wind energy Surface and upper-air tropical and mid-latitude weather systems,

including prevailing westerlies Mesoscale Great Plains Low-Level Jet and nocturnal LLJs Sea-breeze Monsoon circulation Off-shore resources US wind resource maps Forecasting wind resources Atmospheric boundary layer Structure and diurnal/seasonal evolution Impact of static and dynamic stability on horizontal wind speeds

and vertical profiles Turbulent flows and interactive wakes

http://eesc.columbia.edu/courses/ees/climate/lectures/gen_circ/index.html

Not to scale!

Mean radius of the earth:

6371 kmHeight of the troposphere:

0-7 km at poles20 km at Equator

90% of atmosphere is in the lowest 15 miles (24 km)99% in lowest 30 miles (48 km)

Non-rotating Earth heated at its Equator

Global Precipitation Patterns

NOAA NCEP-NCAR CDAS-1 MONTHLY 300 mb [ u , v ] climatology

January

Wind speed at 12 km

NOAA NCEP-NCAR CDAS-1 MONTHLY 300 mb [ u , v ] climatology

July

http://eesc.columbia.edu/courses/ees/climate/lectures/gen_circ/300mbWinds.html

Wind speed at 12 km

NOAA NCEP-NCAR CDAS-1 MONTHLY Diagnostic above_ground [ u , v ] climatology (m/s)

January

http://eesc.columbia.edu/courses/ees/climate/lectures/gen_circ/300mbWinds.html

Wind speed near surface

NOAA NCEP-NCAR CDAS-1 MONTHLY Diagnostic above_ground [ u , v ] climatology (m/s)

July

http://eesc.columbia.edu/courses/ees/climate/lectures/gen_circ/300mbWinds.html

Wind speed near surface

NOAA NCEP-NCAR CDAS-1 DAILY300 mb height (m) and winds (m/s)1 Apr 1997

http://eesc.columbia.edu/courses/ees/climate/lectures/gen_circ/300mbWinds.html

Continental and Regional influences Continental scale circulation, jet streamsGreat Plains Low-Level JetNocturnal LLJCoastal JetsSea breezesMountain-valley flowsMountain compression of stream linesOff-shore wind

Mechanism of Low-Level Jets:

General PrinciplesGreat Plains Low-Level Jet (GPLLJ)

Nocturnal Low-Level Jet (LLJ)Coastal Jet (CJ)

Mechanism of Low-Level Jets:

General PrinciplesGreat Plains Low-Level Jet (GPLLJ)

Nocturnal Low-Level Jet (LLJ)Coastal Jet (CJ)

HLPressure Gradient

HLPressure Gradient

Fc

Fp

Fc = -2ΩxV

Coriolis Force

HLPressure Gradient

Fc

Fp

HLFp Fc

Vg

Geostrophic Balance

HLFp

Fc

V

FfFrictional Force

Ff = -CdvV

HLFp

Fc

V

At night, friction is eliminated, flow is accelerated, V increases

HLFp

Fc

V

Coriolis force increase, wind vector rotates and speed continues to increase

HLFp

Fc

VVg

Wind vector rotates and speed continues to increase and exceeds geostrophic wind

Mechanism of the Nocturnal Low-Level Jet:

General PrinciplesGreat Plains Low-Level Jet (GPLLJ)

Nocturnal Low-Level Jet (LLJ)Coastal Jet (CJ)

Rocky Mountains

Missouri River

High Temp Low TempLow Press High Press

H

Bermuda High creates flow from the south in summer over the central US, which is accelerated at night by a terrain-induced pressure gradient

Wind speed as a function of height during the LLJ peak on March 24, 2009 at 1000 LST from the Lamont, OK wind profiler (Adam Deppe MS thesis, ISU, 2011)

Heig

ht a

bove

gro

und

Horizontal wind speed

Great Plains Low-Level Jet Maximum (~1,000 m above ground)

~1 km

Mechanism of the Nocturnal Low-Level Jet:

Great Plains Low-Level Jet (GPLLJ)Nocturnal Low-Level Jet (LLJ)

Coastal Jet (CJ)

High Temp Low Temp

Low Press High Press

HLFp

Fc

VVg

Heig

ht a

bove

gro

und

Horizontal wind speed

Nocturnal Low-Level Jet Maximum (~400 m above ground)

~400 m

Mechanism of the Nocturnal Low-Level Jet:

Great Plains Low-Level Jet (GPLLJ)Nocturnal Low-Level Jet (LLJ)

Coastal Jet (CJ)

High Temp Low Temp

Low Press High Press

Coastal Mountains

High Temp Low Temp

Low Press High Press

HLFp

Fc

V

FfFrictional Force

Ff = -CdvV

Mountains producean additional pressure force

Heig

ht a

bove

gro

und

Horizontal wind speed

Coastal Jet Maximum (~50-400 m above ocean)

~50-400 m

Note high winds at mountain ridges

100 km

Musial, W., and B. Ram, 2010: Large-scale Offshore Wind Power in the United States. Assessment of Opportunities and Barriers. NREL/TP-500-40745. 240 pp. [Available online at http://www.osti.gov/bridge]

Take Home MessagesWinds are created by horizontal temperature

difference (which create density differences and hence pressure differences)

Rotation of the Earth creates bands of high winds (prevailing westerlies) at mid-latitudes

Interactions with the day-night heating and cooling of

the earth’s surface create changes in the vertical structure of the horizontal wind

Orographic feature (coastal regions, mountains, etc) create local circulations that enhance or decrease wind speeds

Wind Science 101II. Atmospheric Boundary Layer

Eugene S. TakleProfessor

Department of AgronomyDepartment of Geological and Atmospheric Science

Director, Climate Science ProgramIowa State University

Ames, IA 50011

Honors Wind SeminarIowa State University

Spring 2011

High Interannual Variability:Number of Wind Speed Reports per Month

≤ 5 kts at Mason City, IA 1 Oct 2001 – 30 Sep 2002 1 Jan – 31 Dec 1998

Data by Adam Deppe

1 knot= 1.151 mph= 0.514 m/s

Num

ber o

f Occ

urre

nces

Winspeed (m/s)

2 10864 12 14 16 18 20 22

Heig

ht (z

)

Windspeed

Power Law

Logarithmic Dependence

U* = friction velocityk = von Karman’s constant (0.40)zo= roughness length

High Interannual Variability:Number of Wind Speed Reports per Month

≤ 5 kts at Mason City, IA 1 Oct 2001 – 30 Sep 2002 1 Jan – 31 Dec 1998

Data by Adam Deppe

Modeling the Atmospheric Boundary Layer

In Tensor Notation:

K = constant

One-and-a-half order:

Turbulence options:

ε = dissipation

Turbulence Kinetic Energy:

Third Order:

ε = q3/Λ

Conceptual Model of Turbine-Crop Interaction via Mean Wind and Turbulence Fields

__ ___________________________________

Speed recovery

CO2H2O

Heat

day

nightA conceptual model of turbulence generated by turbines suggests enhancement of near-surface mixing both day and night, which will…

reduce daytime maximum temperature in the crop (good)increase night-time temperature in the crop (???)reduce dew-duration in crops (good)enhance downward CO2 flux into the canopy during daytime photosynthesis (good)enhance CO2 flux out of the canopy at night (???)suppress early killing frost (good)help dry down the crop before harvest (good)

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