Page 198 - Satellite Communications, Fourth Edition
P. 198

Chapter Six
                              178
                              178  Chapter Six
                                                                Microstrip feeder



                              Patch antenna




                                                                          Dielectric substrate
                                                                     Ground plane
                                                       (a)


                                                   Radiated fields
                                                              Patch




                                                       (b)
                              Figure 6.29 A patch antenna.

                              itself, and the feed arrangement, but the principles of operation can be
                              understood from a study of the basic patch radiator. In Fig. 6.29a the
                              feed is a microstrip line connecting to the patch, and the copper on the
                              underside of the board forms a ground plane. The dielectric substrate
                              is thin (less than about one-tenth of a wavelength) and the field under
                              the patch is concentrated in the dielectric. At the edges of the patch the
                              electromagnetic fields are associated with surface waves and radiated
                              waves, the radiation taking place from the “apertures” formed in the
                              substrate between the edges of the patch and the ground plane. The radi-
                              ated fields are sketched in Fig. 6.29b.
                                Figure 6.30 shows the patch of sides a and b situated at the origin of
                              the coordinate system of Fig. 6.3. Approximate expressions for the radi-
                              ation pattern in the principal planes at     0 and     90° are [see
                              James et al., 1981, Eqs. (4.26a and b)]:

                                                                  2  b
                                                g(
,     90 )    cos a   sin 
b          (6.41)
                                                                    l 0
                                                                          2
                                                  g(
,     0)    cos 
 c  sin X d        (6.42)
                                                                  2
                                                                      X
                              where X   ( a/l )sin
, and l is the free space wavelength. Equation (6.42)
                                            0
                                                      0
                              will be seen to be similar to Eq. (6.23). A plot of these functions, for a half
                              wavelength patch is shown in Fig. 6.31. In practice the length of each side
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