Towards improved QPE with a local area X-band radar in the framework of COPS F. Tridon, J. Van Baelen and Y. Pointin Laboratoire de Météorologie Physique,

Slides:



Advertisements
Similar presentations
KIT – die Kooperation von Forschungszentrum Karlsruhe GmbH und Universität Karlsruhe (TH) 5.3 Advantages of a coordinated scanning Doppler lidar and cloud.
Advertisements

Peters Gerhard, Fisher Bernd and Andersson Tage. Boreal Environment Research: 7, , (2002) Rain Observations with a vertically looking Micro Rain.
DYnamical and Microphysical Evolution of Convective Storms Thorwald Stein, Robin Hogan, John Nicol DYMECS.
Contrasting Tropical Rainfall Regimes Using TRMM and Ground-Based Polarimetric Radar Steven A. Rutledge, Robert Cifelli, Timothy J. Lang Colorado State.
7. Radar Meteorology References Battan (1973) Atlas (1989)
Page 1 Operational use of dual- polarisation: lessons learned at Météo France after 8 years of experience at all wavelengths (S / C / X) P. Tabary Météo.
Radar Meteorology Laboratory Rain from Doppler Radar data Prof. LEE, Dong-In 23 November 2000.
Retrieval and Application of Raindrop Size Distributions From Polarimetric Radar and Disdrometer Data for Sub-synoptic Scale Systems Petar Bukovčić 1,3,4,
Evolution of long-axis lake-effect convection during landfall and orographic uplift Profiling radar observations during OWLeS 1 Ted Letcher & Justin Minder.
21 September th Southwest Hydrometeorology Symposium, Tucson, AZ Future QPE: Dual-Pol and Gap-Filler Radars Kevin Scharfenberg University of Oklahoma/CIMMS.
Single Frequency Observations of Warm Clouds and Precipitation Edward Luke with Pavlos Kollias, Frederic Tridon, Stefan Kneifel, and Alessandro Battaglia.
DUAL-POLARIZATION OF WSR-88D NETWORK
Radar-Derived Rainfall Estimation Presented by D.-J. Seo 1 Hydrologic Science and Modeling Branch Hydrology Laboratory National Weather Service Presented.
Matthew Shupe Ola Persson Paul Johnston Cassie Wheeler Michael Tjernstrom Surface-Based Remote-Sensing of Clouds during ASCOS Univ of Colorado, NOAA and.
Precipitation Over Continental Africa and the East Atlantic: Connections with Synoptic Disturbances Matthew A. Janiga November 8, 2011.
Preliminary results with the LaMP X band radar J. Van Baelen¹, Y. Pointin¹, F. Tridon¹, and M. Hagen² 1°/ Laboratoire de Météorologie Physique, Observatoire.
Remote sensing of Stratocumulus using radar/lidar synergy Ewan O’Connor, Anthony Illingworth & Robin Hogan University of Reading.
Contrasting Tropical Rainfall Regimes Using TRMM and Ground-Based Polarimetric Radar by S. A. Rutledge, R. Cifelli, T. Lang and S. W. Nesbitt EGU 2009.
Spatial and temporal variability of drop size distribution from vertically pointing micro rain radar (MRR) Clemens Simmer 1 and Malte Diederich 1 Presented.
COPS-GOP-WS3 Hohenheim 2006_04_10 Micro- Rain- Radar Local Area Weather Radar Cloud Radar Meteorological Institute University Hamburg Gerhard Peters.
1 Radar Displays PPI - Plan position Indicator Maps the received signals on polar coordinates in plan view. The antenna scans 360° at fixed elevation angle.
Surveillance Weather Radar 2000 AD. Weather Radar Technology- Merits in Chronological Order WSR-57 WSR-88D WSR-07PD.
Precipitation over Narrow Mountain Ranges Ethan Gutmann Roy Rasmussen, Greg Thompson, David Gochis, Kyoko Ikeda, Changhai Liu, Jimy Dudhia, Martyn Clark.
Spaceborne Weather Radar
What controls the shape of a real Doppler spectrum?
Spaceborne Radar for Snowfall Measurements
Using NPOL (the NASA S-band polarimetric radar), and a network of 2D video disdrometers for external radar calibration and rain rate estimation, and to.
Delft University of Technology 1 Do eddy dissipation rate retrievals work for precipitation profiling Doppler radar?, CESAR Science Day, June 18th, 2014.
Drop size distribution from WXT weather transmitter? Heikki Pohjola, Application specialist Thanks to Elena.
A Doppler Radar Emulator and its Application to the Detection of Tornadic Signatures Ryan M. May.
CARPE-DIEM 13/6/02, slide 1German Aerospace Center Microwaves and Radar Institute CARPE-DIEM Besprechung Helsinki, June 2004 Ewan.
Validation of TRMM rainfall products at Gadanki T. Narayana Rao NARL, Gadanki K. Nakamura, HyARC, Nagoya, Japan D. Narayana Rao, NARL, Gadanki National.
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.
The three-dimensional structure of convective storms Robin Hogan John Nicol Robert Plant Peter Clark Kirsty Hanley Carol Halliwell Humphrey Lean Thorwald.
Department of Mechanical Engineering The Pearlstone Center for Aeronautical Engineering Studies Ben-Gurion University of the Negev P.O.B. 653, Beer Sheva.
Radar Palet e Home Radar Artifacts Radar Palet e Home Radar Artifacts Analysis & Diagnosis 1 Radar Interpretation Problems Reflectivity.
The new DWD polarimetric weather radar network: a new radar data processing framework and new products Michael Frech 1, Nils Rathmann 2, Jörg Steinert.
Dual-Polarization and Dual-Wavelength Radar Measurements Vivek National Center for Atmospheric Research Boulder, Colorado I.Polarization and dual- wavelength.
Remote Sensing of Precipitation A Look at Radar Now and in the Future Western South Dakota Hydrology Conference 23 April 2009 Darren R. Clabo Institute.
Reflectivity and Radial Velocity
Observation report of MRR (3) Tomoki Koshida Research fellow of OKI/KANAE LAB.
Matthew Shupe Ola Persson Paul Johnston Duane Hazen Clouds during ASCOS U. of Colorado and NOAA.
III) CHARACTERISTICS OF THE ADDED CLUTTER RAIN MeteoSvizzera, 6605 Locarno, Switzerland Simulation.
Observation of MRR Tomoki Koshida Research fellow of OKI/KANAE lab 9/22’04 (Micro Rain Radar)
Comparison of Polarimetric C Band Doppler Radar Observations with Reflectivity Fields obtained at S Band: A Case Study of Water induced Attenuation R.
AQUARADAR -D The effects of inhomogeneous rain drop size distributions (DSDs) in a radar volume Vertical structure of DSD profiles Spectral modes of DSDs.
S. Hachani 1,2,B. Boudevillain 1, Z. Bargaoui 2, and G. Delrieu 1 1 University of Grenoble(UJF/ LTHE ) 2 University Tunis el Manar (ENIT/LMHE) EGU, General.
A comparison of cloud microphysics in deep tropical convection forming over the continent and over the ocean Emmanuel Fontaine 1, Elise Drigeard 1, Wolfram.

INFLUENCE OF NON-UNIFORM BEAM FILLING ON ATTENUATION CORRECTION AT C- AND X-BAND A. BERNE LTHE, Grenoble, France. R. UIJLENHOET HWM Group, Wageningen,
Barcelona Toward an error model for radar quantitative precipitation estimation in the Cévennes- Vivarais region, France Pierre-Emmanuel Kirstetter, Guy.
A Combined Radar-Radiometer Approach to Estimate Rain Rate Profile and Underlying Surface Wind Speed over the Ocean Shannon Brown and Christopher Ruf University.
AQUARadar Identification of temporally stable Z-R relationships using measurements of micro-rain radars M. Clemens (1), G. Peters (1), J. Seltmann (2),
Atmospheric profile and precipitation properties derived from radar and radiosondes during RICO Louise Nuijens With thanks to: Bjorn Stevens (UCLA) Margreet.
Experimental study of the “rain effect” on the mobility distribution of air ions. Experiments with water jet. U. Hõrrak, H. Tammet, E.Tamm, A. Mirme. Institute.
The evaluation of updrafts in the Unified Model using single-Doppler radar measurements Nicol JC a, Hogan RJ b, Stein THM b, Hanley KE c, Lean HW c, Plant.
A modeling study of cloud microphysics: Part I: Effects of Hydrometeor Convergence on Precipitation Efficiency. C.-H. Sui and Xiaofan Li.
Impact of Cloud Microphysics on the Development of Trailing Stratiform Precipitation in a Simulated Squall Line: Comparison of One- and Two-Moment Schemes.
Observations of Specific Differential Phase, KDP Chris Collier Acknowledgements: Lindsay Bennett, Alan Blyth and David Dufton.
1/15 Orographic forcing and Doppler winds, the key for nowcasting heavy precipitation in the mountains Luca Panziera, Urs Germann MeteoSwiss, Locarno-Monti,
A Moment Radar Data Emulator: The Current Progress and Future Direction Ryan M. May.
Experimental study of the “rain effect” on the mobility distribution of air ions. Experiments with water jet. U. Hõrrak, H. Tammet, E.Tamm, A. Mirme.
Chap IV. Fundamentals of Radar Beam propagation
By SANDRA E. YUTER and ROBERT A. HOUZE JR
The DYMECS project A statistical approach for the evaluation of convective storms in high-resolution models Thorwald Stein, Robin Hogan, John Nicol, Robert.
Radar/Surface Quantitative Precipitation Estimation
Precipitation Measurements using Radar
Examples of spectral fields
Spaceborne Radar for Snowfall Measurements
Presentation transcript:

Towards improved QPE with a local area X-band radar in the framework of COPS F. Tridon, J. Van Baelen and Y. Pointin Laboratoire de Météorologie Physique, UMR CNRS/UBP , avenue des Landais, Aubière Cedex, France

Introduction (1) Radar technology: tool for quantitative rainfall measurements Main parameters:  Reflectivity factor : Z (mm 6.m -3 )  Rainrate: R (mm.h -1 )  Drop Size Distribution: DSD (l -1.mm -1 ) Power law relationship: Z = aR b Variability of DSD Use of unique Z-R relationship for one precipitating event

Introduction (2) Objective: Quantitative precipitation estimation on a small catchment basin with a simple scanning X-band radar Use of a nearby vertically looking MicroRain Radar to:  study the properties of precipitation (DSD) with a high resolution  do a classification of different rain regimes within the same precipitating event  derive specific Z-R relationships for these regimes Check the efficiency of these specific Z-R relationships against a single one

X-band radar (9.41GHz) Elevation: 5° High resolution:  Time: 30 s  Azimuth: 2°  Range: 60 m Max range: 20 km

Micro Rain Radar (K-band, 24.1GHz) Doppler spectra of 63 bins (0 to 12 m.s -1 ) over 32 range gates every 10 s Relation between drop diameter and terminal fall velocity (Atlas et al. 1973): Profile of DSD

 Derivation of rain parameters:  Attenuation coefficient  Iterative attenuation correction  Reflectivity factor  Rain rate

June 15, 07 (IOP 3b) Synoptic-scale through moving northeastwardly giving stratiform precipitation with weak showers over the COPS area

DSD temporal evolution Grayscale: Number of raindrops in size interval Bold solid line: Median-volume diameter Thin solid lines: 10th and 90th percentiles of distribution of liquid rain water content over raindrop diameters   measure of the width of the raindrop size distribution

DSD temporal evolution 1 st period: small drops, narrow spectra, high variability 2 nd period: large drops, wide spectra, medium variability 3 rd period: low variability anomaly 1 2 3

Anomaly less visible near the ground MRR measurement issue due to:  strong updraft  heavy attenuation  bad noise level estimation

Z-R relationships GlobalSpecific 1 2 3

Corresponding rainfall RainrateCumulative rainfall MRR estimationGlobal Z-RSpecific Z-R Total rainfall (mm)

August 8-9, 07 (IOP 14b) An intense large-scale precipitating system spread over the COPS area during all the night

DSD temporal evolution 1 st period: medium drops, medium variability 2 nd period: small drops, narrow spectra, low variability 3 rd period: small drops, narrow spectra, medium variability 4 th period: high variability

Z-R relationships GlobalSpecific

Corresponding rainfall RainrateCumulative rainfall MRR estimationGlobal Z-RSpecific Z-R Total rainfall (mm)

Conclusions and perspectives High variability of rain even within a stratiform precipitation system Detection of temporally stable regimes of precipitation with significantly different Z-R relationships Derivation of the equivalent exponential or gamma distribution to explain the difference between the Z-R relationships Next step: apply these specific Z-R relationships on the X-band reflectivity

 Problem: How to detect these regimes with a single parameter X-band radar ? Periods of increasing, stagnating and decreasing intensity can be part of the same temporally stable regime of precipitation Conclusions and perspectives

Thanks for your attention Questions ?