Page 535 - Engineering Electromagnetics, 8th Edition
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CHAPTER 14  ELECTROMAGNETIC RADIATION AND ANTENNAS              517



















                                        Figure 14.3 The polar plot of the
                                        E-plane pattern of a vertical current
                                        element. The crest amplitude of E θs is
                                        plotted as a function of the polar angle
                                        θ at a constant distance r . The locus is
                                        a circle.
                     The relation between these fields is evidently the same as that of a uniform plane wave,
                     which an expanding spherical wave approximates at large radii, and over regions in
                     which 1/r is approximately constant. Specifically,

                                                     (kr >> 1or r >> λ)              (24)
                                       E θs = ηH φs
                         The variation of both radiation fields with the polar angle θ is the same; the fields
                     maximize in the equatorial plane (xy plane) of the current element and vanish off the
                     ends of the element. The variation with angle may be shown by plotting a vertical, or
                     E-plane pattern (assuming a vertical orientation of the current element). The E plane is
                     simply the coordinate plane that contains the electric field, which in our present case,
                     is any surface of constant φ in the spherical coordinate system. Figure 14.3 shows
                     an E-plane plot of Eq. (22) in polar coordinates, in which the relative magnitude of
                     E θs is plotted against θ for a constant r. The length of the vector shown in the figure
                     represents the magnitude of E θ , normalized to unity at θ = 90 ; the vector length is
                                                                       ◦
                     just | sin θ|, and so as θ varies, the tip of the vector traces out a circle as shown.
                         A horizontal, or H-plane pattern may also be plotted for this or more complicated
                     antenna systems. In the present case, this would show the variation of field intensity
                     with φ. The H-plane of the current element (the plane that contains the magnetic field)
                     is any plane that is normal to the z axis. As E θ is not a function of φ, the H-plane
                     plot would be simply a circle centered at the origin.

                        D14.1. A short antenna with a uniform current distribution in air has I 0 d =
                        3 × 10 −4  A · m and λ = 10 cm. Find |E θs | at θ = 90 , φ = 0 , and r =:(a)
                                                                           ◦
                                                                    ◦
                        1 cm; (b)2 cm; (c)20 cm; (d) 200 cm; (e)2m.
                        Ans. 125 V/m; 25 V/m; 2.8 V/m; 0.28 V/m; 0.028 V/m
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