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NREL is a national laboratory of the U.S. Department of Energy, Office of Energy Efficiency and Renewable Energy, operated by the Alliance for Sustainable Energy, LLC.
Sodar & Lidar Activities at NREL
IEA Topical Expert Meeting
“Remote Wind Speed
Sensing Techniques Using
Sodar and Lidar”
Neil Kelley, NWTC
October 15-16, 2009
National Renewable Energy Laboratory Innovation for Our Energy Future
OUTLINE
Applications of Remote Sensing at the NWTC
– Wind Flow Characteristics Research
• Low-Level Jet Research
– Sodar
– Scanning Lidar
• Turbulence Scaling Parameters
– Sodar
– Scanning Lidar
– Evaluation of Remote Sensing Technologies to Provide Local
Atmospheric Conditions for Mesoscale Modeling Initialization
• Sodar
National Renewable Energy Laboratory Innovation for Our Energy Future
Wind Flow Characterization Research
120-m tower
with sonic anemometers at
tower heights of 54-, 67-, 85-,
116-m
Scintec MFAS
medium-range
SODAR
NOAA/ESRL High
Resolution Doppler
Lidar (HRDL)
Lamar Low-Level Jet
Program
Objective: To develop an
understanding of the
influence of nocturnal low-
level jets on the inflow
turbulence environment of
multi-megawatt wind
turbines
Cooperative Program
with
Enron (GE) Wind
NOAA/ESRL
DOE/NREL
National Renewable Energy Laboratory Innovation for Our Energy Future
observed
wind
shear
design
wind
shear
Typical Diurnal Variation in Turbine Inflow on the Great
Plains
Why Worry About Low-Level Jets?
National Renewable Energy Laboratory Innovation for Our Energy Future
Sodar & Applications
Scintec Sodar
– Operating characteristics
• 30 to 500 m height range
• Single and multi-frequency operation
• 20-min averaging 10-min records
• Operated 24/7 during “warm” season for
low-level jets (April – September)
– Measurement Objectives
• Determined frequency, height, and intensity
of low-level jets that have been included in
the NREL TurbSim Stochastic Inflow
Simulator Great Plains Spectral Model
• Documented intensity of vertical shears
from 30 to 200 m
• Provided vertical wind direction profiles for
alignment of NOAA HDRL Lidar
National Renewable Energy Laboratory Innovation for Our Energy Future
Examples of Results Derived from Sodar
Observed Distributions of Lowest Jet Maximum Velocities
with Height at Colorado Green Wind Energy Site
Lowest jet height velocity, UHmax
(m/s)
5 10 15 20 25 30
Lowestjetheight,AGL(m)
100
200
300
400
500
100
200
300
400
500
mean
median
5-95% percentiles
Frequency Distribution of Observed Lowest Jet Heights
Lowest jet height, AGL (m)
50 100 150 200 250 300 350 400 450 500
(n/N)(%)
0
1
2
3
4
5
6
Frequency Distribution of Observed Lowest
Jet Height Wind Direction
Lowest jet maxium wind direction (deg)
0 45 90 135 180 225 270 315 360
(n/N)(%)
0
2
4
6
8
10
12
14
10-minute mean wind speed (m/s)
6 8 10 12 14 16 18 20 22
Height(m)
50
100
150
200
250
300
350
400
450
500
02:40
02:50
03:00
03:10
03:20
03:30
03:40
03:50
04:00
Low-Level Jet
Wind Speed
Profile
National Renewable Energy Laboratory Innovation for Our Energy Future
What About Shears Below the Jets?
Vertical Speed Shear Probability Distributions
50m to Height of Lowest Jet
0 2 4 6 8 10 12 14 16 18 20
Percentprobability
0.01
0.05
0.1
0.2
0.5
1
2
5
10
20
mean
maximum
UH shear between 50m and Zjet (m/s/100m)
Vertical Wind Direction Shear Probability Distributions
50m to Height of Lowest Jet
WD vertical shear between 50m and Zjet [deg/(Zjet - 50m)]
-20 -15 -10 -5 0 5 10 15 20Percentprobability
0.05
0.1
0.2
0.5
1
2
5
10
20
30
50
mean
maximum
National Renewable Energy Laboratory Innovation for Our Energy Future
Volumetric Scanning Lidars Used
HRDL technical parameters#
Wavelength 2.02 µm
Pulse energy 1.5 mJ
Pulse rate 200/s
Range resolution 30 m
Velocity resolution ~ 0.1 m/s
Time resolution 0.25 s
Minimum range 0.2 km
Maximum range 3 km
Beam width range 6 to 28 cm
NOAA/ESRL Pulsed Doppler
Coherent Research Lidar
WindTracer® technical parameters#
Wavelength 2 µm
Pulse energy 2 mJ
Pulse rate 500/s
Range resolution 80 m
Velocity resolution 0.1-0.6 m/s
Time resolution 0.1 s
Minimum range 0.4 km
Maximum range 8-10 km
Beam width 8 cm
Lockheed-Martin/CTI Pulsed
Doppler Coherent Lidar
#~as deployed at the NWTC, currently available
model has somewhat different specifications
#as configured for the NREL Lamar
Low-Level Jet Program
National Renewable Energy Laboratory Innovation for Our Energy Future
Examples of Results Derived from HDRL Lidar Using
Different Scanning Modes During Lamar Experiment
NOAA HRDL presentations courtesy R. Banta and Y. Pichugina, ESRL
Vertical sector scan (slices)
Fixed-beam or stare “scan”
Conical scans
“streets” of
coherent
turbulent
structures
Low-Level
Jet
Turbine
Heights
GE 1.5 MW
Turbine
With a bit of signal
processing we can now
see the vertical details
of the coherent
turbulent structures
National Renewable Energy Laboratory Innovation for Our Energy Future
Examples of Results Derived from the WindTracer
Lidar at the NWTC Using a Volume Scan
Frehlich, R. and Kelley, N., 2008
LIDAR NWTC TOWER
Profiles of Turbulence Scaling Parameters
Observed Above the NWTC
Very useful for determining initial conditions for NWP
National Renewable Energy Laboratory Innovation for Our Energy Future
Evaluation of Remote Sensing Technologies for NWP Initialization
– The NWTC presents a challenging environment for sodar observations
particularly if a high data capture is desired for wind speeds within a
overall wind turbine operating range of 3 to 25 m/s.
– Because the wind industry is using low-range or “mini-sodars”, we have
been evaluating a Scintec SFAS sodar because of its high degree of
flexibility including user-selected multi-frequency and multi-beam
operation.
– We conducted an experiment last winter in which the SFAS sodar was
operated over a desired height range of 20-235 m in three separate
configurations:
• 3 frequencies (2549, 3386, and 4479 Hz using 9 radiated beams
• Single frequency (4479 Hz) using 9 radiated beams
• Single frequency (4479 Hz) using 3 radiated beams
Sodar
National Renewable Energy Laboratory Innovation for Our Energy Future
Maximum Altitude Performance Example
with high S/N Ratio
10-Minute Averaging
Percent UH(z) Raw Data Capture Using Default Settings
Percent data captured
0 20 40 60 80 100
Height,AGL(m)
0
50
100
150
200
250
3 frequencies, 9 beam
single frequency, 9 beam
single frequency, 3 beam
National Renewable Energy Laboratory Innovation for Our Energy Future
References
Banta R.M., Y.L. Pichugina, N.D Kelley, B.J. Jonkman, and W.A. Brewer, 2008: Doppler
lidar measurements of the Great Plains low-level jet: Applications to wind energy. 14th
International Symposium for the Advancement of Boundary layer Remote Sensing, 23-
25 June, Risø National Laboratory, DTU, Roskilde, Denmark, pp.4
Kelley, N., M. Shirazi, D. Jager, S. Wilde, J. Adams, M. Buhl, P. Sullivan, and E.
Patton, 2004: Lamar Low-Level Jet Project Interim Report, NREL/TP-500-34593.
Frehlich, R., Kelley, N., 2008: Measurements of Wind and Turbulence Profiles with
Scanning Doppler Lidar for Wind Energy Applications, IEEE Journal of Selected
Topics in Applied Earth Observations and Remote Sensing, 1, 42-47.

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Sodar and lidar activities at nrel, iea r&d wind annex xi expert meeting, nrel, oct 15 16,2009

  • 1. NREL is a national laboratory of the U.S. Department of Energy, Office of Energy Efficiency and Renewable Energy, operated by the Alliance for Sustainable Energy, LLC. Sodar & Lidar Activities at NREL IEA Topical Expert Meeting “Remote Wind Speed Sensing Techniques Using Sodar and Lidar” Neil Kelley, NWTC October 15-16, 2009
  • 2. National Renewable Energy Laboratory Innovation for Our Energy Future OUTLINE Applications of Remote Sensing at the NWTC – Wind Flow Characteristics Research • Low-Level Jet Research – Sodar – Scanning Lidar • Turbulence Scaling Parameters – Sodar – Scanning Lidar – Evaluation of Remote Sensing Technologies to Provide Local Atmospheric Conditions for Mesoscale Modeling Initialization • Sodar
  • 3. National Renewable Energy Laboratory Innovation for Our Energy Future Wind Flow Characterization Research 120-m tower with sonic anemometers at tower heights of 54-, 67-, 85-, 116-m Scintec MFAS medium-range SODAR NOAA/ESRL High Resolution Doppler Lidar (HRDL) Lamar Low-Level Jet Program Objective: To develop an understanding of the influence of nocturnal low- level jets on the inflow turbulence environment of multi-megawatt wind turbines Cooperative Program with Enron (GE) Wind NOAA/ESRL DOE/NREL
  • 4. National Renewable Energy Laboratory Innovation for Our Energy Future observed wind shear design wind shear Typical Diurnal Variation in Turbine Inflow on the Great Plains Why Worry About Low-Level Jets?
  • 5. National Renewable Energy Laboratory Innovation for Our Energy Future Sodar & Applications Scintec Sodar – Operating characteristics • 30 to 500 m height range • Single and multi-frequency operation • 20-min averaging 10-min records • Operated 24/7 during “warm” season for low-level jets (April – September) – Measurement Objectives • Determined frequency, height, and intensity of low-level jets that have been included in the NREL TurbSim Stochastic Inflow Simulator Great Plains Spectral Model • Documented intensity of vertical shears from 30 to 200 m • Provided vertical wind direction profiles for alignment of NOAA HDRL Lidar
  • 6. National Renewable Energy Laboratory Innovation for Our Energy Future Examples of Results Derived from Sodar Observed Distributions of Lowest Jet Maximum Velocities with Height at Colorado Green Wind Energy Site Lowest jet height velocity, UHmax (m/s) 5 10 15 20 25 30 Lowestjetheight,AGL(m) 100 200 300 400 500 100 200 300 400 500 mean median 5-95% percentiles Frequency Distribution of Observed Lowest Jet Heights Lowest jet height, AGL (m) 50 100 150 200 250 300 350 400 450 500 (n/N)(%) 0 1 2 3 4 5 6 Frequency Distribution of Observed Lowest Jet Height Wind Direction Lowest jet maxium wind direction (deg) 0 45 90 135 180 225 270 315 360 (n/N)(%) 0 2 4 6 8 10 12 14 10-minute mean wind speed (m/s) 6 8 10 12 14 16 18 20 22 Height(m) 50 100 150 200 250 300 350 400 450 500 02:40 02:50 03:00 03:10 03:20 03:30 03:40 03:50 04:00 Low-Level Jet Wind Speed Profile
  • 7. National Renewable Energy Laboratory Innovation for Our Energy Future What About Shears Below the Jets? Vertical Speed Shear Probability Distributions 50m to Height of Lowest Jet 0 2 4 6 8 10 12 14 16 18 20 Percentprobability 0.01 0.05 0.1 0.2 0.5 1 2 5 10 20 mean maximum UH shear between 50m and Zjet (m/s/100m) Vertical Wind Direction Shear Probability Distributions 50m to Height of Lowest Jet WD vertical shear between 50m and Zjet [deg/(Zjet - 50m)] -20 -15 -10 -5 0 5 10 15 20Percentprobability 0.05 0.1 0.2 0.5 1 2 5 10 20 30 50 mean maximum
  • 8. National Renewable Energy Laboratory Innovation for Our Energy Future Volumetric Scanning Lidars Used HRDL technical parameters# Wavelength 2.02 µm Pulse energy 1.5 mJ Pulse rate 200/s Range resolution 30 m Velocity resolution ~ 0.1 m/s Time resolution 0.25 s Minimum range 0.2 km Maximum range 3 km Beam width range 6 to 28 cm NOAA/ESRL Pulsed Doppler Coherent Research Lidar WindTracer® technical parameters# Wavelength 2 µm Pulse energy 2 mJ Pulse rate 500/s Range resolution 80 m Velocity resolution 0.1-0.6 m/s Time resolution 0.1 s Minimum range 0.4 km Maximum range 8-10 km Beam width 8 cm Lockheed-Martin/CTI Pulsed Doppler Coherent Lidar #~as deployed at the NWTC, currently available model has somewhat different specifications #as configured for the NREL Lamar Low-Level Jet Program
  • 9. National Renewable Energy Laboratory Innovation for Our Energy Future Examples of Results Derived from HDRL Lidar Using Different Scanning Modes During Lamar Experiment NOAA HRDL presentations courtesy R. Banta and Y. Pichugina, ESRL Vertical sector scan (slices) Fixed-beam or stare “scan” Conical scans “streets” of coherent turbulent structures Low-Level Jet Turbine Heights GE 1.5 MW Turbine With a bit of signal processing we can now see the vertical details of the coherent turbulent structures
  • 10. National Renewable Energy Laboratory Innovation for Our Energy Future Examples of Results Derived from the WindTracer Lidar at the NWTC Using a Volume Scan Frehlich, R. and Kelley, N., 2008 LIDAR NWTC TOWER Profiles of Turbulence Scaling Parameters Observed Above the NWTC Very useful for determining initial conditions for NWP
  • 11. National Renewable Energy Laboratory Innovation for Our Energy Future Evaluation of Remote Sensing Technologies for NWP Initialization – The NWTC presents a challenging environment for sodar observations particularly if a high data capture is desired for wind speeds within a overall wind turbine operating range of 3 to 25 m/s. – Because the wind industry is using low-range or “mini-sodars”, we have been evaluating a Scintec SFAS sodar because of its high degree of flexibility including user-selected multi-frequency and multi-beam operation. – We conducted an experiment last winter in which the SFAS sodar was operated over a desired height range of 20-235 m in three separate configurations: • 3 frequencies (2549, 3386, and 4479 Hz using 9 radiated beams • Single frequency (4479 Hz) using 9 radiated beams • Single frequency (4479 Hz) using 3 radiated beams Sodar
  • 12. National Renewable Energy Laboratory Innovation for Our Energy Future Maximum Altitude Performance Example with high S/N Ratio 10-Minute Averaging Percent UH(z) Raw Data Capture Using Default Settings Percent data captured 0 20 40 60 80 100 Height,AGL(m) 0 50 100 150 200 250 3 frequencies, 9 beam single frequency, 9 beam single frequency, 3 beam
  • 13. National Renewable Energy Laboratory Innovation for Our Energy Future References Banta R.M., Y.L. Pichugina, N.D Kelley, B.J. Jonkman, and W.A. Brewer, 2008: Doppler lidar measurements of the Great Plains low-level jet: Applications to wind energy. 14th International Symposium for the Advancement of Boundary layer Remote Sensing, 23- 25 June, Risø National Laboratory, DTU, Roskilde, Denmark, pp.4 Kelley, N., M. Shirazi, D. Jager, S. Wilde, J. Adams, M. Buhl, P. Sullivan, and E. Patton, 2004: Lamar Low-Level Jet Project Interim Report, NREL/TP-500-34593. Frehlich, R., Kelley, N., 2008: Measurements of Wind and Turbulence Profiles with Scanning Doppler Lidar for Wind Energy Applications, IEEE Journal of Selected Topics in Applied Earth Observations and Remote Sensing, 1, 42-47.