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SOLUTION OF BASIC EQUATIONS OF ELECTRODYNAMICS                          181


                                                    1
                                                = =  =  [s]                     (4.63)
                                                  2  
            4.  The equity (, ) =  −  defines the phase, i.e. space-time phase shift or delay of the
               expending EM wave of single frequency. In general, the phase distribution at any fixed
               moment of time   is characterized by its phase wavefront meaning the position of the
                              
               surface on which the phase of a wave is constant or

                                               −  = .                 (4.64)
                                                
                   Drop a pebble in a calm pond and you get a two-dimensional circular wave on the surface
                   of the pond running outward and forming the pattern likewise in Figure 4.2.3.

            5.  According to (4.61) and (4.64) the surfaces of constant field intensity and phase    coincides
               at  any fixed moment of time. Figure 4.2.3 illustrating (4.64) at an arbitrary but  fixed
               moment of time is, evidently, the dissection of the spheres shown sketchy in Figure 4.2.4a
                                                            5
               and is the resemblance of the Chinese ivory Puzzle Ball  displayed in Figure 4.2.4b.  It is
               clear that the shape of each phase wavefront is an ideal sphere. That is why the waves are
               radiated by the infinitesimal radiator can be called spherical.















                                                     a)                          b)
            Figure 4.2.4. a) Several consecutive images of phase wave front, b) Chinese ivory Puzzle Ball

            6.  The remarkable fact  is  that  the far-away EM  waves emitted by  any  type  of  finite-size
               radiators or finite set of such radiators are obligated to be very close to spherical. To prove
               it assume that the observation points  ≫  . As such, | −  | ≅ (1 −  ∘  ) (see
                                                   ′
                                                                                  ′
                                                                   ′
                                                                              0
               Figure 4.1.1) for any point   inside  .  Physically it means that we measure the fields
                                               ′
                                       ′
               created by an arbitrary antenna in so called far-field zone. For modern antennas such as
               large and  ultra large  radio telescopes,  radars  phased arrays and submarine radio
               communication antenna ground systems this zone can be tens or even hundreds kilometers
               far-off. As a matter of fact, Green’s function in (4.55) is independent of the variable  .
                                                                                    ′
                                                        ′
                                                 �− � |− |�  �− � �
                                         ′                �  0 ∘ ′         (4.65)
                                    (,  , ) =  ≅ 
                                                      ′
                                                   |− |      
            Thus this factor can be pulled outside of the integral in (4.56)
            5  Public Domain Image, source: https://www.pinterest.com/pin/503066220849382214/
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