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Chapter 5                                                               207

               and Direct Broadcast Satellites (DBS)  mainly  use dual  polarization to increase their
               channel capacity (see  statement 2 above).  Unfortunately,  CP  is  more affected by
               atmospheric conditions than LP for high rainfall rates (greater than 12.5 mm/h) and low
               angles of arrival.


            The reader may find much more detailed information about polarization in specialized literature
            [31, 32].




            5.2 ANTENNA PARAMETERS
            5.2.1   Introduction

            Good understanding of the essence of antenna parameters is a vital aspect of the engineering
            experience that  makes  you  be  prepared better for quite challenging  modern antenna
            development. Sometimes such understanding is more important than an in-depth knowledge of
            antenna theory  itself  because  current engineering practice  has  shifted  to “off-the-shelf”
            approach. Consequently, an engineer spends more time increasingly looking through antenna
            catalogs and manuals than on antenna development itself.
            5.2.2   Radiation Resistance and Lumped Equivalent Circuit of Antenna

            Looking back at expression (4.72) from Chapter 4 we can detect surprising parallels with (3.11).
            Both describe the power defined by energy conversion from one form into another. It is clear
            that the RF generator connected to  a  dipole  (see Figure 4.2.1b) delivers and supports  the
            current    . Then   is the power radiated by the dipole, i.e. roughly speaking, the power lost
                        Σ
            by dipole forever in an unbounded medium. If so, the expression in (4.72) can be rewritten as
                                                           2
                                       1                ∆
                                   = (   2  2   2   (5.8)
                                                                )
                                            )  = 40 � � (
                                   Σ       Σ             
                                       2                
            Here   is customarily called radiation resistance, caused by the radiation EM energy from a
                 Σ
            dipole antenna, and equal to
                                                2          2
                                              ∆
                                     = 80 � � ≅ 800 � � [Ω]                   (5.9)
                                                         ∆
                                            2
                                     Σ
                                                     
            The imaginary or quadrature part of the reactive power ℑ( ) concentrated near a dipole ( ≪
                                                           
            ) can be derived in a similar manner and obtained from (5.20) below
                                                             2
                                        1   2  5    ∆   2
                               ℑ( ) = (   )  ≅ − � � � � (   )
                                  
                                                Σ
                                        2                 �             (5.10)
                                                        2
                                                10   ∆
                                          ≅ −  � � � �
                                           Σ
                                                    
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