Preparation of the ADM-Aeolus mission using 355nm high spectral resolution Doppler LIDAR and a Doppler cloud radar

Similar documents
Airborne wind lidar campaigns for preparation of the Aeolus mission Oliver Reitebuch

Contribution of French research teams to ADM Cal/Val

Airborne Coherent Wind Lidar measurements of vertical and horizontal wind speeds for the investigation of gravity waves

High Resolution Sea Surface Roughness and Wind Speed with Space Lidar (CALIPSO)

Benjamin Witschas. Keywords: Coherent Laser Radar, Vertical wind speed, GW-LCYCLE, Deepwave, Airborne Wind Lidar

13.6 AIRBORNE RADAR OBSERVATIONS OF BREAKING WAVES/ROTORS IN THE LEE OF THE MEDICINE BOW MOUNTAINS IN SE WYOMING, USA

Assessing the quality of Synthetic Aperture Radar (SAR) wind retrieval in coastal zones using multiple Lidars

The Sea surface KInematics Multiscale (SKIM)

WindProspector TM Lockheed Martin Corporation

Reprocessed QuikSCAT (V04) Wind Vectors with Ku-2011 Geophysical Model Function

P2.17 OBSERVATIONS OF STRONG MOUNTAIN WAVES IN THE LEE OF THE MEDICINE BOW MOUNTAINS OF SOUTHEAST WYOMING

Workshop on Short-Term Weather Forecasting for Probabilistic Wake-Vortex Prediction. WakeNet3-Europe DLR Oberpfaffenhofen, Germany

Increased Project Bankability : Thailand's First Ground-Based LiDAR Wind Measurement Campaign

Development of SAR-Derived Ocean Surface Winds at NOAA/NESDIS

EXTREME WIND GUSTS IN LARGE-EDDY SIMULATIONS OF TROPICAL CYCLONES

SWIFT. The Stratospheric Wind Interferometer for Transport Studies

Towards a consolidated wind reference for assessing scatterometer high and extreme-force wind capabilities

Executive Summary of Accuracy for WINDCUBE 200S

ERS WAVE MISSION REPROCESSING- QC SUPPORT ENVISAT MISSION EXTENSION SUPPORT

ICE INITIATION IN MIXED-PHASE OROGRAPHIC WAVE CLOUDS

Outline Physical Basis Aerosol Products Validation Algorithm Improvements. AEROCOM Meeting CNES, Paris, June 2-3, 2003

LiDAR Application to resource assessment and turbine control

REMOTE SENSING APPLICATION in WIND ENERGY

Sentinel-1A Ocean Level-2 Products Validation Strategy

Hong Kong International Airport North Runway South Runway

Characterization of Boundary-Layer Meteorology During DISCOVER-AQ

DUTCH OFFSHORE WIND ATLAS

CHANGE OF THE BRIGHTNESS TEMPERATURE IN THE MICROWAVE REGION DUE TO THE RELATIVE WIND DIRECTION

Gravity waves and bores. Material kindly provided by Dr. Steven Koch GSD NOAA (Boulder, CO)

SMAP Radiometer-Only Tropical Cyclone Size and Strength

Offshore Wind Turbine Wake Characterization using Scanning Doppler Lidar

SIMON YUEH, WENQING TANG, ALEXANDER FORE, AND JULIAN CHAUBELL JPL-CALTECH, PASADENA, CA, USA GARY LAGERLOEF EARTH AND SPACE RESEARCH, SEATTLE, WA, US

Airborne measurements of gravity wave breaking at the tropopause

Windcube FCR measurements

M. Mikkonen.

Flow analysis with nacellemounted

Axial Base (PN3A) Medium-Power (MP) J-box

Name: Class: Date: Multiple Choice Identify the letter of the choice that best completes the statement or answers the question.

b. What is the x-distance from the foot of the cliff to the point of impact in the lake?

HIGH RESOLUTION WIND RETRIEVAL FOR SEAWINDS ON QUIKSCAT. Jeremy B. Luke. A thesis submitted to the faculty of. Brigham Young University

SENSOR SYNERGY OF ACTIVE AND PASSIVE MICROWAVE INSTRUMENTS FOR OBSERVATIONS OF MARINE SURFACE WINDS

The AirCore Profiler. methods, challenges, applications and updates

SEA SURFACE TEMPERATURE RETRIEVAL USING TRMM MICROWAVE IMAGER SATELLITE DATA IN THE SOUTH CHINA SEA

Physics Waves & Sound

Results for the stratosphere

Air-Sea Interaction Spar Buoy Systems

Global observations of stratospheric gravity. comparisons with an atmospheric general circulation model

IDRA, IRCTR Drizzle Radar: A High Resolution FMCW X-band Doppler Polarimetric Weather Radar

Investigation on Atmospheric Boundary Layers: Field Monitoring and Wind Tunnel Simulation

CONSTRUCTION OF LNG RECEIVING TERMINAL ON THE SAINT LAWRENCE TIDAL CURRENT CONDITIONS IN THE LEVIS AREA

Deep Sea Offshore Wind Power R&D Seminar Trondheim, Jan. 2011

Wave-Phase-Resolved Air-Sea Interaction

AN EXPERIMENTAL INVESTIGATION OF SPILLING BREAKERS

UTLS Asian monsoon anticyclone

Mesoscale air-sea interaction and feedback in the western Arabian Sea

EVALUATION OF ENVISAT ASAR WAVE MODE RETRIEVAL ALGORITHMS FOR SEA-STATE FORECASTING AND WAVE CLIMATE ASSESSMENT

Physical Science 1 Chapter 6 WAVES. A wave is a disturbance that is propagated through a system. Waves transfer energy.

3D Nacelle Mounted Lidar in Complex Terrain

Study of wake vortex roll up spiral geometry based on real conditions airport Doppler Radar Trials

Analysis of the Radar Doppler Signature of a Moving Human

Strengthening of the tropopause inversion layer during the 2009 sudden stratospheric warming in the MERRA-2 analysis

07/23/02 FC: All aircraft suppressed day hoping for late take-off

Monitoring Conditions Offshore with Satellites

MISR CMVs. Roger Davies and Aaron Herber Physics Department

Exploration Series. HOT AIR BALLOON Interactive Physics Simulation Page 01

Chapter 19: Vibrations And Waves

1. Which one of the following is a vector quantity? A. time B. speed C. energy D. displacement

PRELIMINARY STUDY ON DEVELOPING AN L-BAND WIND RETRIEVAL MODEL FUNCTION USING ALOS/PALSAR

1. A cannon shoots a clown directly upward with a speed of 20 m/s. What height will the clown reach?

Satellite information on ocean vector wind from Scatterometer data. Giovanna De Chiara

Airborne Remote Sensing of Surface and Internal Wave Processes on the Inner Shelf

Fabry Perot / PDV Comparison. May 24, 2007

Determination Of Nearshore Wave Conditions And Bathymetry From X-Band Radar Systems

7 th International Conference on Wind Turbine Noise Rotterdam 2 nd to 5 th May 2017

High Frequency Acoustical Propagation and Scattering in Coastal Waters

In parallel with steady gains in battery energy and power density, the coming generation of uninhabited aerial vehicles (UAVs) will enjoy increased

Examples of Carter Corrected DBDB-V Applied to Acoustic Propagation Modeling

Kinematics-Projectiles

Honors Assignment - Vectors

Viva TPS. TS11/15 Total Stations Check and Adjust Procedure. October Summary

Abrupt marine boundary layer changes revealed by airborne in situ and lidar measurements

Robin J. Beaman. School of Earth and Environmental Sciences, James Cook University, Cairns, Qld 4870, Australia.

A It is halved. B It is doubled. C It is quadrupled. D It remains the same.

Ongoing research in Hong Kong has led to improved wind shear and turbulence alerts

Relative Motion. A look at "Frames of Reference" Website

Introduction to Waves & Sound

High Ping Rate Profile Water Mode 12

Outline Chapter 7 Waves

An algorithm for Sea Surface Wind Speed from MWR

Physics 1520, Spring 2014 Quiz 1A, Form: A

Physics 1520, Spring 2014 Quiz 1B, Form: A

Observations of Gap Flow in the Wipp Valley on 20 October 1999: Evidence of Subsidence

Unit 10 Waves Review Section 1: Know the definitions and/or concepts of the following:

Satellite Observations of Equatorial Planetary Boundary Layer Wind Shear

TRMM TMI and AMSR-E Microwave SSTs

JET PROPULSION LABORATORY INTEROFFICE MEMORANDUM

The MEDUSA Deep Sea and FUSION AUVs:

Assessing Compliance with United States Government Orbital Debris Mitigation Guidelines

Crave the Wave, Feb 16, 2008 TEAM Mentor Invitational Score Rank

LiDAR My favourite tool in the bag 2011 St Kitts & Nevis

Transcription:

Preparation of the ADM-Aeolus mission using 355nm high spectral resolution Doppler LIDAR and a Doppler cloud radar Abdanour Irbah*, Jacques Pelon*, Julien Delanoë*, Gwendal Rivière +, Didier Bruneau*, Quitterie Cazenave* %, Mathilde Van Haecke* and Frédéric Blouzon @ In collaboration with the DLR Team EARTHCARE RALI NAWDEX EPATAN - ESA Contract No. 4000119015/NL/CT/g WindVal II ESA Contract No. 4000114053/15/NL/FF/gp CNES EECLAT INSU/Météo-France ANR-DIP NAWDEX *LATMOS, + LMD, % DLR, @ DT-INSU EGU April 8 13, 2018

Context Infer clouds and aerosol dynamics using airborne RADAR-LIDAR measurements LIDAR-Doppler (HSR LNG), RADAR (RASTA) and Dropsonde measurements were performed during the Iceland NAWDEX/EPATAN campaign LNG performed nadir wind measurements and at 37 off vertical during specific flights to simulate ADM-Aeolus observations Prepare future ADM mission : science and CAL/VAL operations in collaboration with DLR Present our airborne RADAR-LIDAR platform for cloud/aerosol dynamics First results obtained from airborne data recorded during the Iceland campaign RADAR and LIDAR wind measurements; assessment of retrieval uncertainties 2

ADM-Aeolus mission (https://directory.eoportal.org/web/eoportal/satellite-missions/a/aeolus) Main objective: wind profile measurements for studying the dynamics of the atmosphere. Observations will be performed with the Doppler Wind Lidar (ALADIN) at 355 nm. Wind measurements will be obtained from Doppler shifts of backscattered lights by aerosols, clouds and molecules. (image credit: ESA) (image credit: ESA) 3

NAWDEX/EPATAN Iceland campaign 2016: North Atlantic Waveguide Downstream and impact Experiment (Schäfler et al. 2018) / Earthcare PreparATion campaign Exploring the impact of diabatic processes on disturbances of the jet stream and their influence on downstream high-impact weather Prepare EarthCare: joint leg with radar and lidar and A-Train overpasses The French Airborne RAdar-LIdar platform (RALI) was deployed on the French SAFIRE F20 during the Iceland campaign for studying the microphysics and the dynamic of cloud and aerosols. From 28 th of September to 17 th of October 2016 Number of scientific flights: 15 Number of scientific flight hours: 46.5 Number of released dropsondes: 59 Number of CloudSat-CALIPSO overpasses: 3 Number of co-located flights: 5 4

Aircraft: French F20 Payload - RALI Dassault Falcon 20 (SAFIRE) Endurance: 3.5 flight hours Maximum cruising altitude: 13 km Payload: High Spectral Resolution Doppler LIDAR (355 nm), 532 and 1064 nm @ 37 and nadir pointing Doppler Cloud Radar (95 GHz) 3 antennas looking down IR radiometer CLIMAT (nadir brightness temperature 8-10-12 microns) LW/SW fluxes Dropsonde launching (profiles of T, p, RH, u, v) Aircraft measurements (attitude, wind, T, p, RH) LNG (ND : YAG pulsed 20Hz) Wavelength (nm) measurements 355 β, High spectral resolution (MZI), δ, Doppler 532 Backscatter only 1064 Backscatter only 3 antennas RASTA characteristics Frequency (GHz) 95 (3.2 mm) Vertical resolution (m) 60 Horizontal resolution (m) 225 to 300 depending on aircraft speed Range (km) 15 Integration time (ms) 250 (measurement every 750ms for each antenna) Energy (kw) 2 (pulse 0.4μs) Ambiguous velocity (m s -1 ) 8 Antenna size (cm) 45 (0.5 beam width) Sensitivity at 1km (dbz) Down backward: ~-22 / Nadir: ~-30 / Down transverse: ~-26 5

Radial wind measured with LNG in ADM mode Data recorded October 2, 2016 with LNG in ADM (37 ) mode are considered. LNG radial wind => corrected from ground motion (aircraft velocity). dropsonde trajectory LNG measurements during dropsonde s fall-time. Example of radial wind measurements recorded with LNG Oct 2, 2016. 6

Dropsonde and aircraft trajectories Aircraft was flying perpendicular to the wind direction => Wind and LOS almost collinear Wind direction (black vectors) and speed are measured by the dropsonde over a limited field (left). The LNG Light-Of-Sight (red vectors in right side) covers a larger field during the dropsonde fall time. 7

Wind measurements from the dropsonde and LNG Wind speed in the horizontal plane from LNG (r) and dropsonde (b) 40 V (b) and U (g) wind components from dropsonde - LNG wind projections (r) 40 35 30 wind speed (m/s) 30 25 20 15 Vent (m/s) 20 10 0 Meridional and Zonal winds components differ as expected 10-10 5-20 0 0 2 4 6 8 10 12-30 0 2 4 6 8 10 12 Altitude (km) Altitude (km) Dropsonde horizontal wind speed recorded by the dropsonde (black) and LNG (red): they are very closes although the vertical wind component is neglected. 8

Differences of wind speed measurement between LNG and dropsonde 1/2 Wind speed difference versus altitude considering all dropsondes released during the ADM flight of Oct. 2, 2016. Wind speed (m/s) 02-Oct-2016 ADM: Difference between LNG and dropsonde wind components in the horizontal plane 15 10 5 0-5 -10-1 0 1 2 3 4 5 6 7 8 Altitude (km) 100 Error between LNG and dropsonde wind components in the horizontal plane Errors are small between 4 and 7 km, becoming greater at lower altitudes (lower SNR) Error (%) 50 0-50 -1 0 1 2 3 4 5 6 7 8 Altitude (km) 9

Histogram of wind speed differences between LNG and dropsonde 2/2 25 02-Oct-2016 ADM: value histogram of wind speed differences between LNG and dropsonde Histogram of wind speed differences between LNG and dropsondes is not symmetric (not enough samples and error greater at lower altitudes): a small bias is then observed: 0.7 +/- 2.6 m/s occurrence (%) 20 15 10 5 0-10 -5 0 5 10 Wind speed (m/s) 10

RASTA WIND retrieval assessment RASTA against DS (all flights) We use the dropsonde launch time with a 10s window for RASTA measurements Radar reflectivity Vertical velocity Horizontal Wind speed Horizontal Wind direction Wind speed: 0.07 +- 4.06 m/s Wind direction: -3.97 +- 16.53 (Outliers not removed) As a function of altitude 11

Wind speed from LNG, RASTA and Dropsondes 40 Wind component in the horizontal plane from LNG (r), RASTA (g) and dropsonde (b) wind (m/s) 35 30 25 20 15 Wind from LNG (r), RASTA (g) and dropsonde (b): a good agreement is observed. 10 5 0 2 4 6 8 10 12 Altitude (km) Radar data may be considered for comparison when no dropsonde during LNG measurements. A synergistic study of concomitant measurements may be performed. 12

LNG Doppler assessment using ground echo and RASTA Surface velocity (corrected for aircraft s motion) Co-located RASTA wind retrieval (U,V,W) => simulate LNG LOS Ratio < 10 : Bias +- std = 0.28 +-17.50 m/s Ratio > 10 : Bias +- std = 0.09 +-10.88 m/s Bias +- std = 0.05 +- 2.78 m/s Bias +- std = 0.04+- 2.97 m/s 13

summary Ongoing data analysis of RALI observations performed during the Iceland EPATAN/NAWDEX campaign The slant-viewing LNG observations were used to mimic those from ADM-Aeolus: comparisons of retrieval started with dropsondes and radar wind measurements The results obtained from (LNG ADM) flights data recorded on October 2, 2016 were very closes with those obtained with RASTA and recorded with dropsondes. This study revealed: A promising synergy between LNG and RASTA observations in semi-transparent clouds for cloud studies and validation of ADM-AEOLUS Powerful instrumentation on-board the F20 for studying dynamics of aerosol and clouds 14