Page 240 - Analog and Digital Filter Design
P. 240

Impedance Matching Networks















                      Bandpass Matching into a Single Reactance Load
                      One of the most conmon impedance matching problems is to match a resistive
                      source into a load comprising a resistance and a parallel capacitance. If  the load
                      capacitor  can  be  somehow absorbed  into  the  matching  network  design, the
                      problem then reduces to simple resistive matching. A suitable matching network
                      in this case will have a shunt capacitance across the load terminals. This could
                      be a lowpass PI network, or a type-A lowpass L network.

                      There is a simple condition for being able to match a resistive source to a load
                      comprising a resistance and a parallel capacitance. It is that the shunt capaci-
                      tance of  the load must be smaller than the shunt capacitance of  the matcbing
                      network. The circuit is designed to match the source and load resistance. This
                      design produces a certain value of load shunt capacitance. If the load is applied.
                      the capacitance of  the load and the capacitance of  the matching network add
                      together, giving too great a value. This can be corrected by subtracting the load
                      capacitance from the shunt capacitance of  the matching circuit. Thus the load
                      capacitance forms part of the resistive impedance matching circuit.

                      Using  [he load  to form part  of  the  impedance matching circuit is  known as
                      parasitic  absorption.  The diagram  in  Figure  8.9 illustrates the principle. The
                      load is the parallel circuit of  R load and  C load. The terminating capacitor in
                      the  matching  PI network  shown is  calculated  to  be  C term,  by  taking  into
                      account only the resistance of  the source and load. This is reduced in value to
                      allow for the parallel load capacitor, and its value becomes Cterrn minus Cload.



                                                         C = Cterm - Cload
                                                             \                          I




                Figure 8.9
                Parasitic AbsorDtion


                       For example, suppose the shunt capacitor of  an impedance matching network
                      has a value of  lOOpF for matching to a purely resistive load of  75Q. Suppose.
   235   236   237   238   239   240   241   242   243   244   245