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1 Wave Polarization, Polarimetric SAR, and Polarimetric Scattering Models Yisok Oh Dept. of Radio Engineering, Hong-Ik University 다음은 PACRIM Training Course (Workshop) 의 강의 Note 중에서 1.1 Wave Properties 만을 발췌한 것으로, 전파의 성질을 이해하는데 도움이 될 것입니다. Seoul National University, February 16-19, 2000
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2 Contents 1.Wave Polarization 1.1 Wave Properties 1.2 Polarization Synthesis 2.Polarimetric Radar System 2.1 A Scatterometer System 2.2 NASA/JPL POLSAR System 3.Polarimetric Scattering Models 3.1 Surface Scattering 3.2 Volume Scattering
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3 1.1 Wave Properties -. What is the “ Field ” ? -. Waves : Electromagnetic Waves by Maxwell -. Planewave Propagation in free space -. Polarization : Basic concepts -. Microwave Generation : DC to AC -. Microwave Guidance by Waveguides/ Trans. lines -. Microwave Radiation by Antennas -. EM Wave Reflection from infinite planes -. Microwave Scattering from -. Point Targets -. Distributed Targets
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4 Electromagnetic Fields Fields: Spatial distribution of a physical quantity. Static Fields No time-variation Separation of Electric Field and Magnetic Field Electromagnetic Fields Time-varying Fields Dynamic Fields Co-existence of Electric and Magnetic fields : DC: AC
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5 Electrostatic Fields E : Electric Field (showing flux lines) Assuming infinite plates, V Conducting Plates E d +-+- Direction of E : From + charges to - charges
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6 Magnetostatic Fields IEEE Emblem I : Current H : Magnetic Field (showing flux line) voltage current Electric Fields Magnetic Fields Assuming an infinite current line, I H Direction of H : Right-hand rule,
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7 Dynamic (Time-Varying) Fields Electromotive Force (Voltage Source) Conduction Current Displacement Current Maxwell ’ s Equations Time-varying Electric Field E(r,t) Time-varying Magnetic Field H(r,t)
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8 Waves Consider Water wave in a pond. Cut water surface at once (t=t 0 ) with Kwan-Woo ’ s Sword (청룡언월도) and look X (Spatial Displacement) Wave Height Log the height of Fishing Buoy (x=x 0 ) as a time function t (Time) Wave Height Even though the wave comes toward me, the water doesn ’ t !
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9 Electromagnetic (EM) Waves An Example of an EM wave: Magnitude (source, distance, etc.) Sinusoidal Wave Time Variation Z-directed propagation Vector (Polarization) Time z, distance
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10 Phase Velocity = constant Same Phase Assume these circles are surfing boards. Phase velocity = velocity of the equi-phase point Poynting Vector: : Real Power Flow (Magnitude and Direction)
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11 Time-Harmonic Fields Time-harmonic Assumption: Time variation (Maxwell Equation) z : wave prop. direction (Phasor form)
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12 Planewave Propagation x y z HyHy ExEx Planewave: wavefront is plane Spherical wave near an antenna Approximate Planewave in the Far-zone Z-directed propagating Linear polarized (x-direction) Wave
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13 Polarization : shape of the locus of the E vector tip at a given point in space as a function of time. Polarization Linear Circular Elliptical Other Cases ConditionsExamples
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14 Exercise (determination of polarization) Find polarization of the wave, Find instantaneous electric field: Plot electric field: Determine polarization 2 1 Ex Ey Linear pol. with
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15 Polarization Ellipse Lin. Pol. Circular Pol. = Rotation Angle = Ellipticity Angle
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16 Various Polarization States Left Circular pol. Wave directionThumb Electric FieldOther fingers of left hand
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17 Microwave Generation Oscillators TubesSolid State Klystron TWT Magnetron Gunn Diode MESFET HEMT, etc. High Power Light, Cheap D.C. Power Microwave (A.C.) Instability Resonator Amplifying A MESFET Oscillator:
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18 Microwave Guidance Two Conductors Single Conductor No Conductor ( Transverse ElectroMagnetic) Waveguides Coaxial Cable Two-wire Microstrip Rectangular, Circular Waveguides Dielectric Waveguide TEM wave TE, TM waves (Optical fibers) E H direction A Coaxial Cable :
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19 Microwave Radiation Dipole Antenna : Transmission Line (Wave guider) Radiator (Discontinuity) * Current : temporal Variation of charges
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20 Antennas Wire Antenna Aperture Antenna Reflector Antenna Printed Antenna Microstrip Antenna Coaxial Cable Electric Field Lines
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21 EM Wave Reflection x z Perpendicular Polarization Electric field is perpendicular to the incidence plane x z Parallel Polarization Electric field is parallel to the incidence plane Horizontal Polarization Electric field is horizontal to Earth surface Vertical Polarization Magnetic field is horizontal to Earth surface Infinite plane
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22 Microwave Scattering Radar System Radar System Point Target Distributed Target where : Radar Cross Section : Scattering Coefficient
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