Page 79 - Circuit Analysis II with MATLAB Applications
P. 79

Half-Power Frequencies - Bandwidth



         By definition, the half-power frequencies Z 1   and Z 2  in Figure 2.12 are the frequencies at which the
         magnitude of the input admittance of a parallel resonant circuit, is greater than the magnitude at res-

         onance by a factor of  2 , or equivalently, the frequencies at which the magnitude of the input
         impedance of a parallel resonant circuit, is less than the magnitude at resonance by a factor of  2  as
         shown above. We observe also, that Z 1  and Z 2   are not exactly equidistant from Z 0 . However, it is
         convenient to assume that they are equidistant, and unless otherwise stated, this assumption will be
         followed in the subsequent discussion.

         We call Z 1   the lower half-power point, and Z 2  the upper half-power point. The difference Z –  Z 1  is
                                                                                              2
         the half-power bandwidth BW , that is,


                                      Bandwidth =   BW =   Z –  Z                              (2.29)
                                                             2   1
         The names half-power frequencies and half-power bandwidth arise from the fact that the power at
                                                  2
         these frequencies drop to 0.5   since    2 2    =  0.5 .
                                               e
         The bandwidth BW    can also be expressed in terms of the quality factor   as follows:
                                                                            Q
         Consider the admittance

                                                       §
                                                              1 ·
                                             Y =  G +  j ZC –  -------
                                                       ©     ZL  ¹
                                      Z
                                       0 ·
                                   §
         Multiplying the   term by G ----------  , we get
                        j
                                   ©  Z G  ¹
                                      0
                                                     ZZ C      Z
                                                    §
                                                        0
                                                                 0
                                         Y =  G +  jG -------------- –  ------------------  ·
                                                    ©  Z G   ZZ LG  ¹
                                                       0
                                                                0
         Recalling that for parallel resonance
                                                    Z C       1
                                                      0
                                             Q    =  ---------- =  --------------
                                               0P
                                                     G      Z LG
                                                             0
         by substitution we get
                                                        Z
                                                            ------
                                       Y =  G 1 +  jQ 0P §  ©  ------ –  Z 0 ·                 (2.30)
                                                        Z
                                                         0   Z ¹
         and if Z   Z =  , then
                     0
                                                    Y =  G




        Circuit Analysis II with MATLAB Applications                                            2-13
        Orchard Publications
   74   75   76   77   78   79   80   81   82   83   84