Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 A study of range resolution effects on accuracy and precision of velocity.

Slides:



Advertisements
Similar presentations
Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapor and Vertical Humidity Fluxes.
Advertisements

Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity.
Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity.
Optical Properties of Aerosol Particles Introduction Atmospheric aerosol particles play a significant role in determining Earth's climate, through their.
7. Radar Meteorology References Battan (1973) Atlas (1989)
Lecture 12 Content LIDAR 4/15/2017 GEM 3366.
Calibration Scenarios for PICASSO-CENA J. A. REAGAN, X. WANG, H. FANG University of Arizona, ECE Dept., Bldg. 104, Tucson, AZ MARY T. OSBORN SAIC,
Working group on space-based winds January 27-30, 2009 Destin, FL Sara C. Tucker, Wm. Alan Brewer, Scott Sandberg, Mike Hardesty CIRES, University of Colorado.
Atmospheric structure from lidar and radar Jens Bösenberg 1.Motivation 2.Layer structure 3.Water vapour profiling 4.Turbulence structure 5.Cloud profiling.
Balloon-Borne Sounding System (BBSS) Used for atmospheric profiling Measures P, T, RH, wind speed and direction Uncertainties arise from incorrect surface.
Satellite Remote Sensing of Surface Air Quality
Ben Kravitz November 5, 2009 LIDAR. What is LIDAR? Stands for LIght Detection And Ranging Micropulse LASERs Measurements of (usually) backscatter from.
1 Satellite Remote Sensing of Particulate Matter Air Quality ARSET Applied Remote Sensing Education and Training A project of NASA Applied Sciences Pawan.
Lidar remote sensing for the characterization of the atmospheric aerosol on local and large spatial scale.
Aircraft spiral on July 20, 2011 at 14 UTC Validation of GOES-R ABI Surface PM2.5 Concentrations using AIRNOW and Aircraft Data Shobha Kondragunta (NOAA),
Application of a High-Pulse-Rate, Low-Pulse-Energy Doppler Lidar for Airborne Pollution Transport Measurement Mike Hardesty 1,4, Sara Tucker 4*,Guy Pearson.
1 Satellite Remote Sensing of Particulate Matter Air Quality ARSET Applied Remote Sensing Education and Training A project of NASA Applied Sciences Pawan.
Science Objectives for the ATHENA-OAWL Venture Tech Airborne Mission M. Hardesty CIRES University of Colorado/NOAA S. Tucker and C. Weimer Ball Aerospace.
(#694) Monitoring the Hawaii Volcano Plume From Satellite By John Porter School of Ocean Earth Science and Technology, University of Hawaii, Honolulu,
Application of Satellite Data to Particulate, Smoke and Dust Monitoring Spring 2015 ARSET - AQ Applied Remote Sensing Education and Training – Air Quality.
Characterization of Aerosol Physical, Optical and Chemical Properties During the Big Bend Regional Aerosol and Visibility Observational Study (BRAVO) Jenny.
The Importance of Atmospheric Variability for Data Requirements, Data Assimilation, Forecast Errors, OSSEs and Verification Rod Frehlich and Robert Sharman.
Determination of the optical thickness and effective radius from reflected solar radiation measurements David Painemal MPO531.
1 Satellite Remote Sensing of Particulate Matter Air Quality ARSET Applied Remote Sensing Education and Training A project of NASA Applied Sciences Pawan.
A DEPLOYABLE MODULAR WIND PROFILER RADAR FOR LOWER ATMOSPHERE APPLICATIONS William Brown, Steve Cohn, Brad Lindseth National Center for Atmospheric Research.
Scaling Surface and Aircraft Lidar Results for Space-Based Systems (and vice versa) Mike Hardesty, Barry Rye, Sara Tucker NOAA/ETL and CIRES Boulder, CO.
1 Relating Aerosol Profile and Column Measurements to Surface Concentrations: What Have We Learned from Discover-AQ? Raymond Hoff University of Maryland,
Introduction Acknowledgements Funding for the CSU-MAPS is provided through a joint NSF-MRI R 2 grant (AGS# , ) awarded to San Francisco and.
Wu Sponsors: National Aeronautics and Space Administration (NASA) Goddard Space Flight Center (GSFC) Goddard Institute for Space Studies (GISS) New York.
RAdio Detection And Ranging. Was originally for military use 1.Sent out electromagnetic radiation (Active) 2.Bounced off an object and returned to a listening.
The Second TEMPO Science Team Meeting Physical Basis of the Near-UV Aerosol Algorithm Omar Torres NASA Goddard Space Flight Center Atmospheric Chemistry.
1 Satellite Remote Sensing of Particulate Matter Air Quality ARSET Applied Remote SEnsing Training A project of NASA Applied Sciences Pawan Gupta Satellite.
RICO Modeling Studies Group interests RICO data in support of studies.
WEATHER SIGNALS Chapter 4 (Focus is on weather signals or echoes from radar resolution volumes filled with countless discrete scatterers---rain, insects,
1 Atmospheric profiling to better understand fog and low level cloud life cycle ARM/EU workshop on algorithms, May 2013 J. Delanoe (LATMOS), JC.
Airborne Measurement of Horizontal Wind and Moisture Transport Using Co-deployed Doppler and DIAL lidars Mike Hardesty, Alan Brewer, Brandi McCarty, Christoph.
Numerical simulations of optical properties of nonspherical dust aerosols using the T-matrix method Hyung-Jin Choi School.
More on Wind Shear Statistics: Intercomparison of Measurements from Airborne DWL and Ground-based Sensors S. Greco and G.D. Emmitt Simpson Weather Associates.
C. J. Senff, R. J. Alvarez II, R. M. Hardesty, A. O. Langford, R. M. Banta, W. A. Brewer, F. Davies, S. P. Sandberg, R. D. Marchbanks, A. M. Weickmann.
NASA ESTO ATIP Laser Sounder for Remotely Measuring Atmospheric CO 2 Concentrations 12/12/01 NASA Goddard - Laser Remote Sensing Branch 1 James B. Abshire,
There was a notable difference in atmospheric ozone concentrations during the cruises. The lowest ozone mixing ratios were measured in the Southern Atlantic.
Data was collected from various instruments. AOD values come from our ground Radiometer (AERONET) The Planetary Boundary Layer (PBL) height is collected.
Image structures: rain shafts, cold pools, gusts Separate rain fall velocity from air velocity – turbulence retrieval– microphysical retrieval Diurnal.
CLOUD PHYSICS LIDAR for GOES-R Matthew McGill / Goddard Space Flight Center April 8, 2015.
Preliminary comparison results of the October 2003 experiment with GroundWinds NH and NOAA's mini-MOPA lidar S. Tucker 1,2, I. Dors 3, R. Michael Hardesty.
Relating Aerosol Mass and Optical Depth in the Southeastern U.S. C. A. Brock, N. L. Wagner, A. M. Middlebrook, T. D. Gordon, and D. M. Murphy Earth System.
NOAA Airborne Doppler Update Mike Hardesty, Alan Brewer, Brandi McCarty and Christoph Senff NOAA/ETL and University of Colorado/CIRES Gerhard Ehret, Andreas.
Jetstream 31 (J31) in INTEX-B/MILAGRO. Campaign Context: In March 2006, INTEX-B/MILAGRO studied pollution from Mexico City and regional biomass burning,
Satellites Storm “Since the early 1960s, virtually all areas of the atmospheric sciences have been revolutionized by the development and application of.
Chemical Data Assimilation: Aerosols - Data Sources, availability and needs Raymond Hoff Physics Department/JCET UMBC.
GWOLF and VALIDAR Comparisons M. Kavaya & G. Koch NASA/LaRC D. Emmitt & S. Wood SWA Lidar Working Group Meeting Sedona, AZ January 2004.
Stratospheric Aerosol Size Distribution Retrievals Using SAGE III Mark Hervig GATS Inc. Terry Deshler University of Wyoming.
ISTP 2003 September15-19, Airborne Measurement of Horizontal Wind and Moisture Transport Using Co-deployed Doppler and DIAL lidars Mike Hardesty,
Kavaya-1 Coherent Doppler Lidar Roadmap to Both the NRC Decadal Survey “Science Demonstration” and “Operational” Missions Michael J. Kavaya Jirong Yu Upendra.
Ship-Based Measurements of Cloud Microphysics and PBL Properties in Precipitating Trade Cumuli During RICO Institutions: University of Miami; University.
UNIVERSITY OF BASILICATA CNR-IMAA (Consiglio Nazionale delle Ricerche Istituto di Metodologie per l’Analisi Ambientale) Tito Scalo (PZ) Analysis and interpretation.
number Typical aerosol size distribution area volume
The study of cloud and aerosol properties during CalNex using newly developed spectral methods Patrick J. McBride, Samuel LeBlanc, K. Sebastian Schmidt,
What Are the Implications of Optical Closure Using Measurements from the Two Column Aerosol Project? J.D. Fast 1, L.K. Berg 1, E. Kassianov 1, D. Chand.
Early VALIDAR Case Study Results Rod Frehlich: RAL/NCAR Grady Koch: NASA Langley.
Presented by: Robyn D. Williams EAS 6410 April 19, 2004
Fourth TEMPO Science Team Meeting
LIDAR Ben Kravitz November 5, 2009.
Visit for more Learning Resources
TIMN seminar GNSS Radio Occultation Inversion Methods Thomas Sievert September 12th, 2017 Karlskrona, Sweden.
ATMOSPHERIC AEROSOL: suspension of condensed-phase particles in air
Group interests RICO data required
PHY Lecture 16 Lidar remote sensing.
GLAS Cloud Statistics and Their Implications for a Hybrid Mission
Group interests RICO data in support of studies
Presentation transcript:

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 A study of range resolution effects on accuracy and precision of velocity estimates Applications of ship-based 2µm Doppler lidar data to space-based lidar performance Sara C. Tucker*, Alan Brewer, Mike Hardesty, Scott Sandberg, Ann Weickmann*, Dan Law Optical Remote Sensing Group, Chemical Sciences Division (CSD) Earth System Research Laboratory, NOAA *Also with: Cooperative Institute for Research in Environmental Science University of Colorado, Boulder, CO, NOAA/ESRL/CSD Working Group on Space-Based Lidar Winds, Snowmass, Colorado, July 17-21, 2007

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 HRDL Winds Characterizations of the Gulf of Mexico and Galveston Bay Aerosol measurements: used to determine the expected levels of return signal available in this region –Closure in aerosol studies at 355 nm using ozone profiling lidar (OPAL), cavity ring-down, and in- situ instruments. Will attempt to scale the backscatter and extinction numbers to HRDL wavelength for comparison studies. –Comparisons with CALIPSO and HSRL Winds and turbulence information: used to determine the potential performance, including errors, based on sample rate/volumes, etc, in space- based Doppler lidar measurements. Cloud coverage: used to determine the percentage of time a satellite can make measurements at each altitude in this area.

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 HRDL wind and aerosol products for understanding Marine Boundary Layers Composite products Horizontal mean wind profiles Profiles of relative aerosol strength and aerosol layering Vertical winds and vertical mixing/turbulence statistics Horizontal (near surface) mixing/turbulence statistics Aerosol and mixed layer (i.e. Boundary layer) heights Wind speed and directional shear profiles Individual Scan Products Boundary layer dynamic features: rolls, surface streaks, thunderstorm outflows, etc Ship/oil-platform plume detection

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 Objective: To study the effect of variability in the small-scale wind fields, and mean wind shear, on expected performance. Reprocess NOAA’s High Resolution Doppler Lidar (HRDL) TexAQS 2006 measurements with 500m range gates and then, look at accuracy and precision of velocity estimates as compared to 30 m products.

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 Accuracy and Precision Accuracy – how far off is the mean? Bias. Precision – what is the standard deviation of the measurements? Averaging more ACFs or Spectra typically means better precision – but may not mean the results are accurate. High accuracy, low precision Low accuracy, high precision

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 System and processing parameters Typical processing 10 lag ACF 30 m range gate =10 averaged ACF/gate  1000 ACF/estimate Reprocessing 10 lag ACF 501 m range gate =167 averaged ACF/gate  16,667 ACF/estimate 3 m sampling (10 ns) 200 ns PW: 30 m 100 pulse averaging Scanning: 5 deg/sec

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 PPI Scan at 45° Elevation: With Shear Mean of 30m data – 500m RG data

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 PPI Scan at 45° Elevation: With Shear Closest 30m data – 500m RG data

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 Resulting Wind Profiles

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 PPI Scan at 45° Elevation: With Shear

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007

Instrument and atmospheric variance profiles Atmospheric vertical variance Wideband SNR Instrument precision

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, m Range Gate Study: Preliminary Results Average SNR usually about the same as 500 m range gates except in cases of strong turbulence and/or approaching “saturation.” Precision Improvements: –16.67 x more points (for a total of 16,667) should yield ~4X improvement in precision – for same SNR. –We see ~2X improvement in precision. In other words, instrument “variance” drops by an average factor of ~4 instead of Profile Wind speed “error”, Mean: m/s, Std. Dev: 0.50 m/s. Profile Wind direction “error”, Mean: 0.34°, Std. Dev: 4.24°. Next for the 500 m. range gate study –Closer look at differences in atmospheric variance estimates – are we underestimating instrument variance? –This study assumed full azimuth scanning at 45° - what happens if we only have 2 stare angles?

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 HRDL-TexAQS 2006: Relative 2µm Aerosol Backscatter Major Saharan dust events

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, µm backscatter True, HRDL was not calibrated for aerosol for TexAQS. HRDL avg. power constant throughout experiment (within 5% error on power-meter measurement). HRDL provided “relative” aerosol layer info during the experiment. In-situ measurements of particle size distribution, composition, absorption, extinction, etc. available Aerosol backscatter is affected by: –Humidity –Composition –Distributions/ Concentration

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 Surface area size distributions and HRDL SNR ABCDE Image credit: D. Coffman, PMEL, NOAA Integrated 2-10µm surface area HRDL SNR at 215 m altitude Correlation ~0.9

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 Particle size distributions: concentrations and backscatter Likely hard target returns

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 Backscatter dependence on RH and Particle Solubility Strong dependence on RH Some dependence on Solubility

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, µm Backscatter: Caveats CNR fit depends on: –Refractive turbulence –Transmission/extinction (estimated in Mie models) Ship plume – strong refractive turbulence Possible long-term system changes due to high vibration Mie scattering models still “young” –Particle refractive index is highly composition dependent): Incorporate variable mass fractions of Ammonium Sulfate, Sea Salt, and Dust

Lidar Working Group on Space-Based Winds, Snowmass, Colorado, July 17-21, 2007 Continuing work Boundary Layer Heights – 600 m over Gulf Streak Analysis and integration of HRDL data with models Comparisons of HRDL with in-situ-based calculations of Backscatter, then… Compare HSRL and CALIPSO and characterize the relationship between 1 and 2 micron backscatter in this area. Extend the process to other areas.