Page 559 - Engineering Electromagnetics, 8th Edition
P. 559

CHAPTER 14  ELECTROMAGNETIC RADIATION AND ANTENNAS              541


                        D14.8. In an endfire linear dipole array in which ξ =−kd, what minimum
                        element spacing d in wavelengths results in bi-directional operation, in which
                        equal intensities occur in the H plane at φ = 0 and φ = π?

                        Ans. d = λ/2

                        D14.9. Fora linear dipole array in which the element spacing is d = λ/4,
                        what current phase ξ will result in a main beam in the direction of a) φ = 30 ;
                                                                                     ◦
                        b) φ = 45 .
                                ◦
                               √       √
                        Ans. −π 3/4; −π 2/4


                     14.7 ANTENNAS AS RECEIVERS

                     We next turn to the other fundamental purpose of an antenna, which is its use as
                     a means to detect, or receive, radiation that originates from a distant source. We
                     will approach this problem through study of a transmit-receive antenna system. This
                     is composed of two antennas, along with their supporting electronics, that play the
                     interchangeable roles of transmitter and detector.
                         Figure 14.16 shows an example of a transmit-receive arrangement, in which the
                     two coupled antennas together comprise a linear two-port network. Voltage V 1 and
                     current I 1 on the antenna at the left affect the voltage and current (V 2 and I 2 )on
                     the antenna at the right—and vice-versa. This coupling is quantified through trans-
                     impedance parameters, Z 12 and Z 21 . The governing equations take the form

                                               V 1 = Z 11 I 1 + Z 12 I 2            (84a)

                                               V 2 = Z 21 I 1 + Z 22 I 2            (84b)
                         Z 11 and Z 22 are the input impedances to antennas 1 and 2 when either antenna is
                     isolated and is used as a transmitter, or equivalently, if the two antennas are sufficiently
                     faraway from each other. The real parts of Z 11 and Z 22 will be the associated radiation






                                      +   I 1                    I 2   +
                                      V 1                            V 2
                                      –                                –
                                            Z 11  Z 21   Z 12  Z 22




                                      Figure 14.16 A pair of coupled antennas,
                                      demonstrating Eqs. (84a) and (84b).
   554   555   556   557   558   559   560   561   562   563   564