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Also,  the  modulating  signal  is  produced  by  frequency  dividing  down  from  the
            10.7386-MHz  crystal  to  generate  an  839-Hz  waveform  at  pin  5  of the  74HC393
            counter.  This  is  done by dividing the 537-kHz signal  from  pin  3 of the  74HC390  by
            5 via  its second  divide-by-5 circuit at pin  7.  The output signal  (537  kHz/5  or 107.4
            kHz)  at  pin  7  of the  74HC390  counter  is  further  divided  by  128  via  binary
            counter/divider  circuit  74HC393,  U4B  cascading  to  U4A  to  produce  an  837-Hz
            square wave  at pin  5 of the 74HC393  counter.  Thus the  modulating waveform  is  a

            triangle  wave  at 839  Hz  across  C4,  which  feeds  into the  load  resistors  R10  and  R5
            to provide pulse amplitude modulation at 455 kHz and  537 kHz,  respectively.
                                                   Chapter 5


                  Low-Power Tuned Radio-Frequeincy Radios



            The  very  first  radios  were  tuned  radio-frequency  (TRF)  radios  back  in  the  early
            twentieth  century.  TRF  radios  were  made  commercially  from  the  beginning  of
            amplitude-modulation  (AM)  radio to the twenty-first century.  As  of 2012,  there are
            still  commercially  made  TRF  radios for the AM  section  of an  AM/FM  radio,  such  as

            the Kaide  Model  KK -205  radio that sells for about $5  to $6  on  eBay.  Also the Kaide
            Model  KK-9 AM/FM/SW (shortwave) radio that sells for about $7 on  e8ay has a TRF
            AM  radio  section  while having  a superheterodyne circuit for the  FM  and  SW  bands.
            This  chapter  will  explore  TRF  radios  that drain  very  little  power,  and  a  number of
            designs will be presented.

                             Design Considerations for TRF Radios

            In  the  world  of  low-power  design,  we  are  talking  about  radios  or  receivers  that
            drain less than  1 mA on  one or two cells.  However, we will set a goal for something
            in  the  range  of less  than  300  ~A. Why  such  a low current consumption?  Well,  the
            milliampere-hour  capacity  of an  AA  alkaline  cell  is  about  2,500  mAh,  whereas  an
            alkaline C cell  has about 7,000 mAh,  and  a D ceU  has about 14,000 mAh.  Thus,  for
            a radio that drains about 300  IJA  continuously,  one  or two D cells  will  last about 5

            years,  whereas a C cell  will go for about 2.5 years,  and  an AA cell will  run  for about
            11  months.
            As  a single-cell  battery drains,  the  voltage  drops from about  1.5 volts to about  1.2
            volts  or  1.1  volts  before  becoming  unusable.  Thus  the  radios  must  work  at the
            lower voltages to extend  useful  battery life.  For the most part,  low-power radios  in
            this  book  shall  drive  crystal  earphones.  Conventional  magnetic  or  dynamic

            earphones  or headphones  normally are  low  resistance  and  require  milliamperes of
            current drive, which thus will shorten battery life considerably.
            Now,  what types  of devices  shall  we  use  for  low-powered  radios?  80th  bipolar
            transistors  (BJTs)  and  field-effect transistors  (FETs)  are  available.  For  the  greatest
            voltage  gain  or  power  gain  per  any  given  operating  current,  bipolar  transistors
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