International Research Centre for Telecommunications and Radar High resolution 3D wind profiling using an S-band polarimetric FM-CW radar: dealiasing techniques.

Slides:



Advertisements
Similar presentations
POLARIMETRIC RADAR IMPROVEMENTS
Advertisements

ATS 351 Lecture 9 Radar. Radio Waves Electromagnetic Waves Consist of an electric field and a magnetic field Polarization: describes the orientation.
Contributors to Measurement Errors (Chap. 7) *1) Widespread spatial distribution of scatterers (range ambiguities) *2) Large velocity distribution (velocity.
Review of the current and likely future global NWP requirements for Weather Radar data Enrico Fucile (ECMWF) Eric WATTRELOT & Jean-François MAHFOUF (Météo-France/CNRM/GMAP)
Matthew Shupe Ola Persson Paul Johnston Cassie Wheeler Michael Tjernstrom Surface-Based Remote-Sensing of Clouds during ASCOS Univ of Colorado, NOAA and.
International Research Centre for Telecommunications and Radar High resolution atmospheric profiling with the S-band Doppler polarimetric radar TARA Christine.
Remote-sensing of the environment (RSE) ATMOS Design of a radar control and signal processor unit for the TARA radar BAP afstudeerproject Yann Dufournet.
Continuing research on radar-observed precipitation systems during NAME 2004 Timothy J. Lang, Stephen W. Nesbitt, Steven A. Rutledge, Robert Cifelli, David.
Atmospheric structure from lidar and radar Jens Bösenberg 1.Motivation 2.Layer structure 3.Water vapour profiling 4.Turbulence structure 5.Cloud profiling.
How can we get a vertical profile of the wind in the atmosphere?
Günther Haase Tomas Landelius Daniel Michelson Generation of superobservations (WP2)
IRCTR: International Research Centre for Telecommunications and Radar Evaluation of particle shape and orientation within ice clouds using the S-band Doppler.
COPS-GOP-WS3 Hohenheim 2006_04_10 Micro- Rain- Radar Local Area Weather Radar Cloud Radar Meteorological Institute University Hamburg Gerhard Peters.
Radar Operations during AMMA SOP Alain Protat  Benin mesosite : Scanning Polarimetric Doppler X-band radar (X-Port) + Scanning Polarimetric Doppler C-band.
Institut für Physik der Atmosphäre POLDIRAD Polarization Diversity Doppler Radar Martin Hagen DLR Oberpfaffenhofen.
Analysis of Three Dimensional Wind Fields from Two Operational Radars Yong Kheng Goh* and Anthony Holt * Doppler radar and wind-field.
Dual-Doppler Wind Retrieval from two operational Doppler radars Yong Kheng Goh, Anthony Holt University of Essex, U. K. for CARPE DIEM, Bologna 29 Nov.
IRCTR - International Research Centre for Telecommunication and Radar ATMOS Ice crystals properties retrieval within ice and mixed-phase clouds using the.
How can we get a vertical profile of the atmosphere?
Doppler Radar From Josh Wurman NCAR S-POL DOPPLER RADAR.
Surveillance Weather Radar 2000 AD. Weather Radar Technology- Merits in Chronological Order WSR-57 WSR-88D WSR-07PD.
What controls the shape of a real Doppler spectrum?
Basic RADAR Principles Prof. Sandra Cruz-Pol, Ph.D. Electrical and Computer Engineering UPRM.
Profilers. Wind profilers are phased array radars that measure the wind as a function of height above a fixed location. Characteristics: Wavelength: 33.
Review Doppler Radar (Fig. 3.1) A simplified block diagram 10/29-11/11/2013METR
Remote-sensing of the environment (RSE) ATMOS Analysis of the Composition of Clouds with Extended Polarization Techniques L. Pfitzenmaier, H. Russchenbergs.
Delft University of Technology 1 Do eddy dissipation rate retrievals work for precipitation profiling Doppler radar?, CESAR Science Day, June 18th, 2014.
Wind Profiler Signal & Data Processing -Anil Anant Kulkarni SAMEER, IIT Campus,Powai Mumbai
A Doppler Radar Emulator and its Application to the Detection of Tornadic Signatures Ryan M. May.
CloudNet: TARA status and database H. Russchenberg, O. Krasnov Delft University of Technology – IRCTR, The Netherlands.
Problems and Future Directions in Remote Sensing of the Ocean and Troposphere Dahai Jeong AMP.
Doppler Radar Basic Principles.
Profilers & Surface Gauges NE Corner of Stuart Hwy & McMillans 2835-MHz Precip. Profiler: km 920-MHz Wind Profiler: km 50-MHz Wind Profiler:
Measurements of raindrop-size distributions from dual-polarization spectral observations Dmitri Moisseev and V. Chandrasekar Colorado State University.
Precipitation studies with RADARS and use of WP/RASS By S.H. Damle.
Cabauw Experimental Site for Atmospheric Research - CESAR - Henk Klein Baltink Atmospheric Research Section.
Simulation of Intense Convective Precipitation Observed during ARMEX Someshwar Das, R. Ashrit, M. Dasgupta, Someshwar Das 1, R. Ashrit 1, M. Dasgupta 1,
Potential Benefits of Multiple-Doppler Radar Data to Quantitative Precipitation Forecasting: Assimilation of Simulated Data Using WRF-3DVAR System Soichiro.
Radar Palet e Home Dual Polarized Analysis & Diagnosis 1 Precipitation Phase – Radar Signatures Radar characteristics of precipitation types –Stratiform.
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.
Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies.
WEATHER SIGNALS Chapter 4 (Focus is on weather signals or echoes from radar resolution volumes filled with countless discrete scatterers---rain, insects,
1 Spectral identification & suppression of ground clutter contributions for phased array radar Spectral identification of ground clutter Spectral identification.
KNMI 35 GHz Cloud Radar & Cloud Classification* Henk Klein Baltink * Robin Hogan (Univ. of Reading, UK)
Atmospheric InstrumentationM. D. Eastin Fundamentals of Doppler Radar Mesocyclone WER Hook Echo Radar ReflectivityRadar Doppler Velocities.
Comparison of Polarimetric C Band Doppler Radar Observations with Reflectivity Fields obtained at S Band: A Case Study of Water induced Attenuation R.
Image structures: rain shafts, cold pools, gusts Separate rain fall velocity from air velocity – turbulence retrieval– microphysical retrieval Diurnal.
Dual-Polarization Radars
Surface Layer SLODAR J. Osborn, R. Wilson and T. Butterley A prototype of a new SLODAR instrument has been developed at Durham CfAI and tested at the Paranal.
ISRO RADAR DEVELOPMENT UNIT, BANGALORE. PRESENTATION TO CHAIRMAN - ISRO & MEMBERS - ISRO COUNCIL NRSA LECTUREGPM – GV MEETING # 2 ISRAD GROUND VALIDATION.
Weather Radars in the US ---- An Overview and Their Applications Cai Huaqing National Center for Atmospheric Research Boulder, CO.
Dual-pol obs in NW Environment B. Dolan and S. Rutledge OLYMPEX planning meeting Seattle, 22 January 2015.
Upper Air Wind Measurements by Weather Radar Iwan Holleman, Henk Benschop, and Jitze vd Meulen Contents: Introduction to Doppler Radar Velocity Azimuth.
Martin Hagen Institut für Physik der Atmosphäre DLR Oberpfaffenhofen Introduction to Meteorological Radars COPS Summer School 2007.
Estimation of Doppler Spectrum Parameters Comparison between FFT-based processing and Adaptive Filtering Processing J. Figueras i Ventura 1, M. Pinsky.
Quality of Weather Radar Wind Profiles Iwan Holleman (KNMI) Introduction of VAD technique in early 60s Development of VVP technique in late 70s Strong.
Statistical Analysis of S-Pol Polarimetric Radar Data from NAME 2004 Timothy J. Lang, Robert Cifelli, Steven A. Rutledge, Angela Rowe, and Lee Nelson Colorado.
presented by: Reham Mahmoud AbD El-fattah ali
A Moment Radar Data Emulator: The Current Progress and Future Direction Ryan M. May.
What is Doppler Weather Radar
A dual-polarization QPE method based on the NCAR Particle ID algorithm Description and preliminary results Michael J. Dixon1, J. W. Wilson1, T. M. Weckwerth1,
Methodology for 3D Wind Retrieval from HIWRAP Conical Scan Data:
Speed simulator / Traceability and Uncertainty Walter Fasel
An overview by: Thomas Jones December 2, 2002
the University of Oklahoma
Doppler Dilemma Ideal in forecasting: Would you settle for:
Examples of spectral fields
Wind Retrieval at Millimeter and Submillimeter Wavelengths
Spaceborne Radar for Snowfall Measurements
Radar-lidar retrievals of water cloud parameters
Presentation transcript:

International Research Centre for Telecommunications and Radar High resolution 3D wind profiling using an S-band polarimetric FM-CW radar: dealiasing techniques Christine Unal, Herman Russchenberg Delft University of Technology, The Netherlands Dmitri Moisseev Colorado State University, Fort Collins, CO, USA  Type of measurement  First main limitation: small Maximum Unambiguous Doppler velocity  Dealiasing techniques (polarimetric and classical)  Example of Wind retrieval results

International Research Centre for Telecommunications and Radar  Goal: Dynamics and Microphysics of Precipitation and Clouds  Sensor: Doppler polarimetric radar TARA (S-band)  High resolution in space (30-3 m) and time (1-10s)  Location: Atmospheric profiling site Cabauw (synergy with other sensors)

International Research Centre for Telecommunications and Radar Measurement configuration 3 beams  3 mean Doppler velocities  horizontal wind + vertical wind 15 o OB1 Y X MB OB o elevation vertical MB VV HV HH OB1 OB2 The max. unambiguous Doppler velocity is reduced by a factor 5 time

International Research Centre for Telecommunications and Radar Polarimetric de-aliasing Expected differential phase ~ 0 at S-band Measured differential phase: Measured Doppler speed Maximum unambiguous Doppler speed Non simultaneity of VV and HH measurements

International Research Centre for Telecommunications and Radar Main beam: polarimetric dealiasing technique  Expected differential phase ~ 0 at S-band  Measured differential phase shows different mean values in case of aliasing

International Research Centre for Telecommunications and Radar Main beam: polarimetric dealiasing technique

International Research Centre for Telecommunications and Radar Main beam: polarimetric dealiasing technique

International Research Centre for Telecommunications and Radar Profiles of mean Doppler velocities for the 3 beams Classical dealiasingPolarimetric dealiasing

International Research Centre for Telecommunications and Radar Resulting horizontal wind retrievals

International Research Centre for Telecommunications and Radar Conclusions  High resolution profiling of horizontal wind in precipitation and clouds example with time resolution = 5 s and range resolution = 30 m  What has still to be done Improved clutter suppression for non polarimetric beams Separation between fall velocities of hydrometeors and vertical wind Correction for effects of beam divergence (possible limitation for high altitudes clouds)  First Objectives Dynamics of the boundary layer. Preparation for study of cloud-aerosol interaction.

International Research Centre for Telecommunications and Radar Main beam: polarimetric dealiasing technique Applying the classification in 5 intervals, the Doppler spectra bins of targets with  co smaller than 0.78 are placed in the wrong interval of Doppler velocities Clutter and noise reduction

International Research Centre for Telecommunications and Radar Offset beam: classical dealiasing technique Precipitation event slant profile Aliased Doppler spectra Doppler velocity [m/s]

International Research Centre for Telecommunications and Radar Offset beam: classical dealiasing technique Resulting spectrograph with dealiasing + noise reduction Search for signal above noise level at Unfolding (using max. spectral reflectivity) Reference: Doppler spectrum of cloud Range continuity check with a cross correlation function