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RADAR METEOROLOGY Yrd. Doç. Dr. Ali DENİZ. OUTLINE INTRODUCTION RADAR HARDWARE ELECTROMAGNETİC WAVES RADAR EQUATION FOR POINT TARGETS METEOROLOGICAL TARGETS.

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Presentation on theme: "RADAR METEOROLOGY Yrd. Doç. Dr. Ali DENİZ. OUTLINE INTRODUCTION RADAR HARDWARE ELECTROMAGNETİC WAVES RADAR EQUATION FOR POINT TARGETS METEOROLOGICAL TARGETS."— Presentation transcript:

1 RADAR METEOROLOGY Yrd. Doç. Dr. Ali DENİZ

2 OUTLINE INTRODUCTION RADAR HARDWARE ELECTROMAGNETİC WAVES RADAR EQUATION FOR POINT TARGETS METEOROLOGICAL TARGETS DISCUSSIONS REFERENCES

3 RA dio D etection A nd R anging LI ght D etection A nd R anging wawelength RADIO RADAR Buderi – 1996 :THE INVENTION THAT CHANGED THE WORLD Young and Taylor – 1934 :PULSES OF ENERGY INTRODUCTION

4 Doppler Radars power speed RADAR DATAAUTOMATIC WARNINGS POLARIZATION KINDS SHAPES SIZES

5 RADAR HARDWARE reflector transmitter modulator Master Clock receiver display antenna waveguide duplexer

6 How Does Radar Work? single antenna target short pulses of energy send Return back The antenna rotates about a vertical axis, scanning the horizon in all directions To determine how high a storm is, met. radars can also aim their antennas above the horizon Whole cycle 10 to 20 elevation angles + 4 to 6 minutes DATA...DISPLAY

7 TYPES OF RADARS Monostatic and Bistatic radar CW and pulsed radar Doppler radar FM-CW radar Wind profilers and aircraft radars Airborn radar Shipboard radar Weather radar Dual-wavelength radar Polarization-diversity radar

8 RADARS USED IN AVIATION ARSR: ASR: TDWR: ARDE: L-band, =20 cm Detect aircraft Provide information on the position of aircrafts Detect microbursts, gustfronts, wind shifts, pecipitaion Follow aircraft on the ground at some airports

9 ELECTRO-MAGNETIC WAVES Radio & radar electro-magnetic radiation f : 1 Hz=1 cycle / second c: m/s : m

10 Elektromagnetic spectrum Skolnik, 1980.

11 Radar bands and corresponding frequency bands, (Rinehart, 2001). Radar BandsFrequencyWavelength HF3-30 MHz100-10 m VHF30-300 MHz10-1 m UHF300-1000 MHz1-0.3 m L1-2 GHz30-15 cm S2-4 GHz15-8 cm C4-8 GHz8-4 cm X8-12 GHz4-2.5 cm Ku12-18 GHz2.5-1.7 cm K18-27 GHz1.7-1.2 cm Ka27-40 GHz1.2-0.75 cm mm or W40-300 GHz7.5-1 mm

12 REFRACTIVE INDEX c : the speed of light in a vacuum u: the speed of light in a medium n: refractive index c  u (always) n  1 (unitless parameter) Actually, it has two components ; k Absorption of coefficient of the medium For air; m=1.003

13 REFRACTIVITY[N] Atm. Press. (mb, hPa) Temp. (°K) Vap. Press. (mb, hPa) Num. of free electron / m 3 Freq. of the radar (Hz.) Under normal atmospheric contions; Ground N Z N

14 RADAR EQUATION FOR POINT TARGET radarstorms Rainrate and... radarPuls of energy into space by antenna Power A spherically expanding shell of energy r : the range from the radar Power density : S

15 The power intercepted bye the target target The amount of energy detected by radar will be: A e : The effective area of the receiving antenna

16 New! THE BACK-SCATTERING CROSS-SECTIONAL CROSS-SECTIONAL AREA OF THE TARGET Final Form SPHERICAL TARGETS A sphere is LARGE “Large” : A sphere is SMALL RAYLEIGH region “Small” :

17 In the Rayleigh region :: related to the complex index of refraction of the material Meteorological targets small RAYLEIGH REGION MET. RADAR USE SOME STANDART POINT TARGETS : Spheres, birds, aircraft, buildings, water towers and radio towers.... In conclusion; Point targets are imp. source of echo for many radars. By making careful measurements of the return from point targets, much canbe learned about the targets. Well-chosen point targets also make it possible to monitor the health and quantitative reliability of a particular radar system. (Battan, 1973)


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