11.07.2015 Views

Principles of Modern Radar - Volume 2 1891121537

Principles of Modern Radar - Volume 2 1891121537

Principles of Modern Radar - Volume 2 1891121537

SHOW MORE
SHOW LESS
  • No tags were found...

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

13.2 Polarization 595Therefore, we examine the locus described by the tip <strong>of</strong> the electric field vector E in theplane z = 0, as time changes, for different values <strong>of</strong> E 0x , E 0y and δ.13.2.1.1 Linear PolarizationWhen the phase difference δ = 2nπ, n an integer, the two components are in phase, andwe have E x /E 0x = E y /E 0y . Thus, the wave is linearly polarized with its locus traversinga positive slope in the first and third quadrants (Figure 13-2a). When the phase differenceis an odd multiple <strong>of</strong> 2π, that is, δ = (2n + 1) π, we have E x /E 0x =−E y /E 0y , and thestraight line locus traverses negative slope in second and fourth quadrants (Figure 13-2b).13.2.1.2 Circular PolarizationWhen the amplitudes <strong>of</strong> the two components in (13.1) are equal (E 0x = E 0y = E 0 ) andthe phase difference δ =±π/2, the electric field is given byE(t) = ˆxE 0 cos(ωt) ∓ ŷE 0 sin(ωt) (13.2)It can be seen that as ωt increases from 0 to 2π, the tip <strong>of</strong> the electric field vectortraverses a circle, and thus the wave is circularly polarized. When δ =+π/2, the tip rotatescounterclockwise with the observer looking into the direction <strong>of</strong> propagation (out <strong>of</strong> thepage in Figure 13-2), and the wave is said to be left-hand polarized. Equivalently, if the lefthandthumb points to the direction <strong>of</strong> propagation while the fingers <strong>of</strong> the left hand curl inthe direction <strong>of</strong> rotation <strong>of</strong> the electric vector, the wave is left-hand polarized. Conversely,the wave is right-hand polarized when the sense is described by right-hand thumb andfingers, as can be verified for the case δ =−π/2. For example, the loci for these twosenses <strong>of</strong> circular polarization are depicted in Figure 13-2c (RCP) and Figure 13-2d (LCP).It may be seen that the tip rotates along the circle <strong>of</strong> radius E 0 with a constant angular rate ω.yyFIGURE 13-2E 0yE 0yEx0x xE 0x(a)(b)yyE 0 Ex 0x(c)(d)yyE 0y E 0yE 0x E 0xxxPolarization statesin a planeperpendicular todirection <strong>of</strong>propagation.(a) linear polarization(LP) with positiveslope. (b) LP withnegative slope.(c) Right circularpolarization (RCP).(d) Left circularpolarization (LCP).(e) Right-handedelliptical polarization(EP). (f) Left-handedEP. The propagationdirection is out <strong>of</strong>the page.(e)(f)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!