Page 316 - Analog and Digital Filter Design
P. 316

Transmission Lines and Printed Circuit Eoards as  Filters   3




                     Suppose you  wish  to design a stripline filter. The problem is that  the  short-
                     circuited line would be very difficult to produce on a printed circuit board. It
                     would be necessary to use a coplanar line (two parallel lines) between the earth
                     planes. An  alternative option is  to  transform  the short-circuited line into an
                     L  structure,  comprising an  open-circuit line  and  a  series section,  Kuroda's
                     identity (see rcference 3) gives the relationship between the two structures and
                     equations have been presented here to simplify the conversion.

                     The open circuit line impedance is given by the equation:

                                    2"
                            Z'  = Z, +-,   where 2 is the value of the short-circuit line impedance
                                     2
                              and Z'  is the replacement open-circuit line value. Z, is the filter's
                              source and load impedance, that is, 50Q.

                           Z'= 50 + 31.25 = 81.25Q.

                           The series section line impedance Z,' is given by  the equation: 2,' = Z,
                             + 2, where 2 is the value of the short-circuit line impedance and 2'
                              is the series section line impedance. As before, Z,, is the filter's source
                             and load impedance. 2,' = 50 + 81.625 = 131.625Q.

                     A diagram of  this filter is given in Figure 12.3. Note that all transmission line
                     sections are a quarter wavelength at the stopband frequency. The width of  the
                     35Q line in the center must not shorten the series section line length. If the pass-
                     band is I .5 GHz and the stopband is at 3 GHz the same impedance can be used,
                     but the length of  the lines must be scaled to be  d/4 at 3GHz instead of  200
                     MHz. The impedance of  the lines is dependent on the passband to stopband
                     ratio rather than the actual frequencies. The velocity of  a wave in a conductor,
                     which is surrounded by a dielectric, is r/&.  Remember that c is the velocity of
                     an electromagnetic wave in free space, and is approximately 3 x 108m/s.
               Figure 12.3  111



                                                   Slohm
                                                                   35ohm
                                                                               Slohm




               Stripline Lowpass Filter             l3lohm           I3lohm


                     The high  impedance line can  be  a  thin  wire.  The impedance of  a  wire  in  a
                     stripline circuit, where there is an earth plane above and below the conductor,
                     is given by:
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