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Inductor-Iess (aka Coil-less) Superheterodyne Radio

            Here  is  a  problem  to  solve:  How  do  you  design  a superheterodyne  radio  without
            any coils?  One way is to substitute every inductor with a gyrator.  Or if a band-pass

            filter is needed, one can  use a ceramic filter or a gyrator.
            But what if you  want to design  an  inductor-Iess superheterodyne  radio  with just a
            one-section  variable  capacitor  or,  better  yet,  tune  the  radio  without  a  variable
            capacitor at all? So this was  what I  was thinking during the last four months before
            I  was  going  to write this  book.  The initial design  was  to use  ceramic filters for the

            IF  stages  and  no  tuned  RF  stage.  This  design  would  work,  except  that  using  a
            455-kHz  ceramic  filter  with  a  single  conversion  RF  mixer  circuit  would  result  in
            receiving  radio signals at image frequencies.
            For example,  without a variable band-pass filter tuned to the desired frequency and
            fed  to the converter or mixer circuit,  an  image signal  will  convert (or mix down) to
            the same  IF frequency  at twice  the  IF frequency  (e.g.,  twice the IF frequency  = 2

            x  455  kHz  = 910  kHz)  plus the frequency of the desired  station. See the following
            table for some examples.



             Desired Station  Frequency       IF Frequency                    Image Frequency
             540  kHz                        455  kHz                         1,450 kHz
             610  kHz                        455  kHz                         1,520 kHz

             680  kHz                         455  kHz                        1,590 kHz
            However,  there  is  another  technique  called  double  conversion that  eliminates
            receiving  stations at the  image frequencies.  But a double-conversion  radio  requires
            a second  mixer or converter circuit and  other IF filters. The double-conversion radio

            is  workable,  but it  was  decided  that the  inductor-Iess  radio design  will  stick to just
            one converter circuit instead.
            Therefore,  to  get around  the  problem  of receiving  stations  at  image  frequencies,
            the  IF  frequency  was  raised  to  about  600  kHz  (or  higher),  and  a  broadband
            low-pass filter was  used to remove signals higher than  1,600 kHz.  Any signal  above
            1,600  kHz  would  be  filtered  out  and  not able  to  mix or  convert  down  to the  new

            600-kHz IF frequency.  See the following table for some examples.



             Desired Station  Frequency       IF Frequency                    Image Frequency
             540  kHz                         600  kHz                        1,740 kHz
             610  kHz                         600  kHz                        1,810 kHz

             680 kHz                          600  kHz                        1,880 kHz
            As  stated  previously,  any signal  above  1,600 kHz  will  be attenuated or removed  by
            a  low -pass  filter.  Figure  11-5  is  a  block  diagram  for  an  inductor-Iess
            superheterodyne  radio.  For  the  antenna,  a short wire  of less  than  2 or 3 feet or a

            telescoping  antenna  will  be  sufficient to pick up  radio  stations in the AM  broadcast
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