Page 29 - Antennas for Base Stations in Wireless Communications
P. 29

2        Chapter One

                  polarization, input impedance, radiation patterns, gain, and efficiency.
                  An antenna in the transmitting mode has a maximum power acceptance.
                  An antenna in the receiving mode differs in its noise rejection proper-
                  ties. The designer should evaluate and measure all of these parameters
                  using various means.

                  1.1.1  Input Impedance
                  and Equivalent Circuits
                  As electromagnetic waves travel through the different parts of the
                  antenna system, from the source (device) to the feed line to the antenna
                  and finally to free space, they may encounter differences in impedance
                  at each interface. Depending on the impedance match, some fraction
                  of the wave’s energy will reflect back to the source, forming a standing
                  wave in the feed line. The ratio of maximum power to minimum power in
                  the wave can be measured and is called the standing wave ratio (SWR).
                  An SWR of 1:1 is ideal. An SWR of 1.5:1 is considered to be marginally
                  acceptable in low-power applications where power loss is more critical,
                  although an SWR as high as 6:1 may still be usable with the right equip-
                  ment. Minimizing impedance differences at each interface will reduce
                  SWR and maximize power transfer through each part of the system.
                    The frequency response of an antenna at its port is defined as input
                  impedance (Z in ). The input impedance is the ratio between the volt-
                  age and currents at the antenna port. Input impedance is a complex
                  quantity that varies with frequency as Z in ( f ) = R in ( f ) + jX in (f), where f
                  is the frequency. The antenna’s input impedance can be represented as
                  a circuit element in the system’s microwave circuit. The antenna can
                  be represented by an equivalent circuit of several lumped elements, as
                  shown in Figure 1.1. In Figure 1.1, the equivalent circuit of the antenna
                                           , with internal impedance, Z = R  + jX . The
                  is connected to a source, V s                      s   s    s
                  antenna has an input impedance of Z  = R a  + jX a . The real part consists
                                                    in




                       X s            R r

                      R s
                                      R l

                       V s
                                      X a

                          Z in
                  Figure 1.1  Equivalent circuit of
                  an antenna
   24   25   26   27   28   29   30   31   32   33   34