Page 484 - Engineering Electromagnetics, 8th Edition
P. 484

466                ENGINEERING ELECTROMAGNETICS















                                         Figure 13.12 Plane wave representation of TE and TM modes in a
                                         parallel-plate guide.


                                     the mode propagates. The TEM mode, however, has no cutoff; it will be supported
                                     at any frequency. At a given frequency, the guide may support several modes, the
                                     quantity of which depends on the plate separation and on the dielectric constant
                                     of the interior medium, as will be shown. The number of modes increases as the
                                     frequency is raised.
                                        So to answer our initial question on the distinction between transmission lines
                                     and waveguides, we can state the following: Transmission lines consist of two or
                                     more conductors and as a rule will support TEM waves (or something which could
                                     approximate such a wave). A waveguide may consist of one or more conductors, or
                                     no conductors at all, and will support waveguide modes of forms similar to those
                                     just described. Waveguides may or may not support TEM waves, depending on the
                                     design.
                                        In the parallel-plate guide, two types of waveguide modes can be supported.
                                     These are shown in Figure 13.12 as arising from the s and p orientations of the plane
                                     wave polarizations. In a manner consistent with our previous discussions on oblique
                                     reflection (Section 12.5), we identify a transverse electric or TE mode when E is
                                     perpendicular to the plane of incidence (s-polarized); this positions E parallel to the
                                     transverse plane of the waveguide, as well as to the boundaries. Similarly, a transverse
                                     magnetic or TM mode results withap polarized wave; the entire H field is in the
                                     y direction and is thus within the transverse plane of the guide. Both possibilities
                                     are illustrated in Figure 13.12. Note, for example, that with E in the y direction
                                     (TE mode), H will have x and z components. Likewise, a TM mode will have
                                                           3
                                     x and z components of E. In any event, the reader can verify from the geome-
                                     try of Figure 13.12 that it is not possible to achieve a purely TEM mode for val-
                                     ues of θ other than 90 . Other wave polarizations are possible that lie between the
                                                       ◦
                                     TE and TM cases, but these can always be expressed as superpositions of TE and
                                     TM modes.



                                     3  Other types of modes can exist in other structures (not the parallel-plate guide) in which both E and
                                     H have z components. These are known as hybrid modes, and they typically occur in guides with
                                     cylindrical cross sections, such as the optical fiber.
   479   480   481   482   483   484   485   486   487   488   489