Page 416 - Engineering Electromagnetics, 8th Edition
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398                ENGINEERING ELECTROMAGNETICS




















                                                      Figure 11.6 Electric field in the xy plane
                                                      of a right circularly polarized plane wave,
                                                      as described by Eq. (98). As the wave
                                                      propagates in the forward z direction, the
                                                      field vector rotates counterclockwise in the
                                                      xy plane.


                                     Choosing +π/2 leads to (97), whose field vector rotates in the clockwise direction.
                                     The handedness of the circular polarization is associated with the rotation and propa-
                                     gation directions in the following manner: The wave exhibits left circular polarization
                                     (l.c.p.) if, when orienting the left hand with the thumb in the direction of propagation,
                                     the fingers curl in the rotation direction of the field with time. The wave exhibits right
                                     circular polarization (r.c.p.) if, with the right-hand thumb in the propagation direc-
                                                                            7
                                     tion, the fingers curl in the field rotation direction. Thus, with forward z propagation,
                                     (97) describes a left circularly polarized wave, and (98) describes a right circularly
                                     polarized wave. The same convention is applied to elliptical polarization, in which
                                     the descriptions left elliptical polarization and right elliptical polarization are used.
                                        Using (96), the instantaneous angle of the field from the x direction can be found
                                     for any position along z through
                                                           E y  
      ∓sin(ωt − βz)
                                            θ(z, t) = tan −1  = tan −1               =∓(ωt − βz)     (99)
                                                          E x          cos(ωt − βz)
                                     where again the minus sign (yielding l.c.p. for positive z travel) applies for the choice
                                     of φ =+π/2in (96); the plus sign (yielding r.c.p. for positive z travel) is used if



                                     7  This convention is reversed by some workers (most notably in optics) who emphasize the importance
                                     of the spatial field configuration. Note that r.c.p. by our definition is formed by propagating a spatial
                                     field that is in the shape of a left-handed screw, and for that reason it is sometimes called left circular
                                     polarization (see Figure 11.7). Left circular polarization as we define it results from propagating a
                                     spatial field in the shape of a right-handed screw, and it is called right circular polarization by the
                                     spatial enthusiasts. Caution is obviously necessary in interpreting what is meant when polarization
                                     handedness is stated in an unfamiliar text.
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