Page 234 - Analog and Digital Filter Design
P. 234

23 1
                                                     Impedance Matching Networks




                Impedance Matching Networks

                      Impedance matching networks are invariably bandpass designs. They are par-
                      ticularly  valuable  at  radio  frequencies (RF) because  even  small circuits can
                      behave like a transmission line. From transmission line theory you may know
                      that  if  a  line is  not  terminated  in  its  characteristic  impedance,  signals are
                      reflected back towards the source.

                      The purpose of  an impedance matching network is to transfer all the available
                      power from a source into a load. Consider a 50Q source matching into a 2OQ
                      load. If  the source EMF (or open circuit voltage) is one volt, and the source
                      is properly matched by  an equal load. 0.5V will be produced across the load.
                      Thus in terms of power transfer, the load should absorb 0.25/50 watts, or 5mW.
                      If  an impedance-matching circuit is  between the source and load, the power
                      into  the  load  should  also  be  5mW.  The  load  voltage  should  therefore  be
                      d(Power x resistance), or d(5.e - 3 x 20) =   = 0.3162V. This is illustrated in
                      Figure 8.7.



                                              Source    Matching Network      Load







                Figure 8.7
                Impedance Matching Principles



                      With  no  matching network in  place the  load  voltage can  be  determined by
                      potential  divider calculations: RLI(RL + RS) = 20170  = 0.2857V.  The power
                      lost by direct connection is not very significant, so at low frequencies it is not
                      usual to provide impedance matching circuits. However, at radio frequencies, the
                      power reflected back towards the source must be minimized to ensure correct
                      operation.

                      For continuous signals the reflection causes a standing wave, which is described
                      by the ratio of  the maxinium to minimum voltages along a line. The incident
                      voltage being added to the reflected voltage causes the maximum voltage; that
                      is, the waves are in phase. The reflected voltage being subtracted from the inci-
                      dent voltage causes the minimum voltage; that is, the waves are anti-phase. High-
                      voltage standing waves (e.g., in radio transmitter circuits) can cause damage to
                      components.  Reflections can  also  cause  distortion  products,  particularly  in
                      mixer and amplifier circuits.
   229   230   231   232   233   234   235   236   237   238   239