Weather Radar SOEE: Lecture 10 Dr Lindsay Bennett
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Who am I? University of Leeds PhD Meteorology 2003-2008 Post-Doctoral Research Assistant 2008-2011 Instrument Scientist National Centre for Atmospheric Science
LECTURE PLAN • History of Radar • General Principles • Reflectivity, Rainrate, Velocity • Nowcasting • Dual Polarisation
History of UK Weather Radar • 1935 Robert Watson-Watt, meteorologist by training, developed the first practical radar system to track aircraft RADAR=RAdio Detection And Ranging • During the war, weather echoes were initially considered a nuisance • 1950s and 60s, first studies of storm dynamics and precipitation forecasting
History of UK Weather Radar • Dee Weather Radar project, 1966-1975 – real time rainfall measurements over the Dee River valley catchment • Network of radars proposed by P.J. Bulman and K.A. Browning in 1971 • North West Radar Project 1976-1984 – first unmanned, automatic radar system at Hameldon Hill, near Burnley
UK Radar network • 4 radars in 1985, 12 by the mid 1990s • Today: 18 radars, 15 operated by the Met Office 5km 2km 1km
How does Radar work? Sends out pulses of electromagnetic radiation in a narrow beam Radiation scatters off targets, some returns to the radar Radar listens for the return pulse Targets can be weather or any physical object
Frequency of Weather Radar High frequency Low frequency 1019 Hz 105 Hz • Weather radar frequencies are usually S,C and X band • Range between f=2-12 GHz (109Hz) (λ=2-15cm), f ~ 1/λ • Microwave energy peak power = 50-500 kW • Microwave oven 2.45 GHz/ λ=12cm, 700 W
Weather Radar Scanning • PPI – Plan Position Indicator • RHI – Range Height Indicator Z X Y X Met Office radars repeat a sequence of several PPIs at different elevation angles every 5 minutes
Weather Radar Scanning • For a radar to locate a target of interest (e.g. rain) 3 pieces of information are needed: range, azimuth and elevation Y R X Speed=distance/time Z Power received Reflectivity Rainrate X Target Velocity Air motions
The Radar Equation • The weather radar equation describes the relationship between: – the transmitted (Pt) and received power (Pr) – the properties of the radar (C) – the properties of the targets (Z) – the distance between the radar and the targets (R) Pt CZ Pr 2 R
Radar Reflectivity • Z, Radar Reflectivity, is a function of target size (D6), number of drops (N) and has units of mm6/m3 6 6 D D=5mm, D =5 = 15,625 D=0.5mm, D6=0.56 = 0.01 D • dBZ (decibels of Z) = 10 log10(Z) • 30 dBZ = 10 X 20 dBZ!!
Reflectivity – Hurricane Katrina
Estimating Precipitation with Radar • Z = f (D6) Reflectivity Z (mm6/m3) is a function of the size of drops (D6) and the number of drops (N) • R = f (D3) Rainfall rate R (mm/hr) is a function of D3, N and the fall speed of the drops (v) • No direct relationship between Z and R • If we assume a distribution of particles (i.e. number of drops in different size categories) we can relate Z to R • Z=ARB R=(Z/A)1/B – Marshall and Palmer (1948) Z=200R1.6 A=200, B=1.6 – hundreds of relationships: depends on rain type (convective, stratiform, mixed), season, location (tropics, mid-latitudes) and cloud type • 30dBZ ~ 2.7mm hr-1 • 60dBZ ~ 205mm hr-1 • Quantitative Precipitation Estimation (QPE) or Forecasting (QPF)
Doppler Velocity • Doppler effect or Doppler shift – change in frequency due to a moving object • Austrian mathematician and physicist, Christian Doppler (1803- 53) • Doppler radar can detect whether a target is moving towards or away from the radar location • Measure the change in the phase of the returned pulses • Calculate Doppler velocity • Met Office radars being upgraded to have Doppler capability
Tornado Signature Reflectivity (dBZ) Radial Velocity (m/s) 5km -6 34 Towards Away Radar location
Clear Air Data • Radar waves scatter off non-meteorological targets too – trees, buildings, power lines are known as “ground clutter” – insects act as “tracers” of the air motion STORM STORM INSECTS INSECTS Radial Velocity (m/s) Reflectivity (dBZ)
Clear Air Data Insects Insects Radial Velocity (m/s) Reflectivity (dBZ)
Nowcasting • Very short-range forecasting • Detailed analysis of current weather situation and forecasting up to 6 hours ahead – track radar echoes and extrapolate into future – combine high resolution numerical forecast models with observational data (satellite, sounding, surface) – UK Met Office Nimrod, Gandolf systems – USA – TITAN, Auto-Nowcaster
Radar Errors • Ground clutter • Strong winds • Attenuation • Evaporation below beam • Bright band • Mixed precipitation (ice and liquid) HAIL Ground Clutter WIND Rain Guage
Bright Band Vertically- pointing radar Height (km) Time (UTC)
Attenuation • Reduction in signal due to scattering and absorption • Worse for shorter wavelengths (X-band)
Dual-polarisation Radar By comparing reflected power returns in different ways (ratios, correlations, etc.), it is possible to obtain information on the size, shape, and ice density of cloud and precipitation particles. Can also correct for errors associated with attenuation and bright band
Differential Reflectivity ZDR ~ log (ZH/ZV) Big drops ZH > ZV, ZDR > 0 Hail ZH=ZV, ZDR=0
Dual-polarisation Radar • http://www.wdtb.noaa.gov/courses/dualpol/animations/PhiDP_animation.html • Horizontal and vertical waves are slowed down (attenuated) different amounts when propagating through precipitation • Radar measures the difference in the phase (phase shift) of the H and V returned pulses • Amount of phase change ~ amount of attenuation ~ intensity of rainfall • Better estimates of rain rate
UK Radar Network • Met Office started upgrade of the network • Doppler by end of 2012 (1-2 weeks downtime) • Dual-polarisation by Autumn 2014 (2-3 weeks downtime)
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