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Dr. S. Cruz-Pol, INEL 4152-Electromagnetics

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Presentation on theme: "Dr. S. Cruz-Pol, INEL 4152-Electromagnetics"— Presentation transcript:

1 Dr. S. Cruz-Pol, INEL 4152-Electromagnetics
Polarization: Why do we care?? Antenna applications – Antenna can only TX or RX a polarization it is designed to support. Straight wires, square waveguides, and similar rectangular systems support linear waves (polarized in one direction, often) Round waveguides, helical or flat spiral antennas produce circular or elliptical waves. Remote Sensing and Radar Applications – Many targets will reflect or absorb EM waves differently for different polarizations. Using multiple polarizations can give different information and improve results. Absorption applications – Human body, for instance, will absorb waves with E oriented from head to toe better than side-to-side, esp. in grounded cases. Also, the frequency at which maximum absorption occurs is different for these two polarizations. This has ramifications in safety guidelines and studies. Cruz-Pol,ECE Dept. UPRM Electrical Engineering, UPRM

2 Dr. S. Cruz-Pol, INEL 4152-Electromagnetics
Polarization In general, plane wave has 2 components; in x & y And y-component might be out of phase wrt to x-component, d is the phase difference between x and y. x y Ey Ex y x Front View Cruz-Pol,ECE Dept. UPRM Electrical Engineering, UPRM

3 Dr. S. Cruz-Pol, INEL 4152-Electromagnetics
Several Cases Linear polarization: d=dy-dx =0o or ±180on Circular polarization: dy-dx =±90o & Eox=Eoy Elliptical polarization: dy-dx=±90o & Eox≠Eoy, or d=≠0o or ≠180on even if Eox=Eoy Unpolarized- natural radiation Cruz-Pol,ECE Dept. UPRM Electrical Engineering, UPRM

4 Dr. S. Cruz-Pol, INEL 4152-Electromagnetics
Linear polarization Front View d =0 @z=0 in time domain x y Ey Ex Back View: y x Cruz-Pol,ECE Dept. UPRM Electrical Engineering, UPRM

5 Circular polarization
Dr. S. Cruz-Pol, INEL 4152-Electromagnetics Circular polarization Both components have same amplitude Eox=Eoy, d =d y-d x= -90o = Right circular polarized (RCP) d =+90o = LCP Cruz-Pol,ECE Dept. UPRM Electrical Engineering, UPRM

6 Elliptical polarization
Dr. S. Cruz-Pol, INEL 4152-Electromagnetics Elliptical polarization X and Y components have different amplitudes Eox≠Eoy, and d =±90o Or d ≠±90o and Eox=Eoy, Cruz-Pol,ECE Dept. UPRM Electrical Engineering, UPRM

7 Parámetros de la elipse
Dr. S. Cruz-Pol, INEL 4152-Electromagnetics Parámetros de la elipse y Eyo a b o x Eyo Cruz-Pol,ECE Dept. UPRM Electrical Engineering, UPRM

8 Polarization Loss Factor PLF
Dr. S. Cruz-Pol, INEL 4152-Electromagnetics Polarization Loss Factor PLF Cruz-Pol,ECE Dept. UPRM Electrical Engineering, UPRM

9 Poincaré Sphere Plots any possible state of polarization
Cruz-Pol,ECE Dept. UPRM

10 Cruz-Pol,ECE Dept. UPRM


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