Page 154 - Build Your Own Transistor Radios a Hobbyists Guide to High-Performance and Low-Powered Radio Circuits
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from  T2's  secondary  winding.  However,  because  the  emitter  of Q2  has  a  24-V

            resistor to ground, the actual  input resistance  is about the transistor's current gain
            (beta  or  Hfe,  typically  100) times  24  V,  which  is  about 2,400  V.  Thus  the  emitter
            24-V resistor  raises  the  input resistance  while  essentially  providing  about the same
            voltage  gain  as  if Q2  were  biased  at (typically)  1 mA  of collector current with  the
            emitter bypassed to ground with a capacitor.
            The  amplified  IF signal then  is connected  to the second  IF transformer T3,  and  the

            secondary  winding  of T3  is  connected  to  D3  for  demodulation  of the  4S5-kHz  AM
            signal.  Because  the  demodulated  AM  signal  is  going  to  be  recirculated  into  the
            converter oscillator transistor Ql, it is essential  to remove any 455-kHz signal  prior
            to connection  to the  base  of Ql via  the secondary winding  of Ll, the antenna  coil.
            Therefore,  a  low-pass  filter  formed  by  C8,  L2,  and  C9  removes  substantially  the

            455-kHz  IF signal  component from  the detector diode  D3  while  coupling  an  audio
            signal to the base of Ql via the secondary winding of Ll.
            At  audio  frequencies,  the  converter  oscillator  circuit  has  an  input  resistance  of
            about 100,000


             (beta times R2  = 1,000


            , where  beta  = 100). The  primary  impedance of T4  is  in  fact about 10  kV  because

            the tapped  secondary of T4  is  being  loaded  by the  input resistance  of Q2,  which  is
            2,400  V.  Recall  that the tapped  secondary winding  of T4  should  be  2,500  V.  Thus
            there  is  close  to an  optimal  power transfer in  impedance  matching  for T4  into Q2,
            and  the aUdio-voltage gain  from  the  base of Ql to the  base  of Q2  is  about 5.  The
            audio gain from the base of Ql to its collector is  10 k



            /1 k


             = 10.  But because the center tap of the secondary of T4  is  used,  we only get half
            the audio-signal voltage, which  is connected to the base of Q2.
            With  the amplified  (T4) audio signal  coupled  to the  base  of Q2,  the collector of Q2
            supplies sufficient current to output transformer TS  for driving  a loudspeaker at its
            secondary  winding.  The  DC  collector  current  of Q2  is  set  at about  15  mA  with  a

            SOO-V  impedance  load  to  allow  for  7.5  volts  peak  or  15  volts  peak  to  peak  of
            alternating-current (AC) signal  swing.  Note that the term impedance is used  instead
            of resistance.  Transformer Ts  allows the audio-signal voltage at the collector of Q2
            to swing  above the 9-volt power supply.  Thus the 15 mA of collector current allows
            the  collector  to  swing  about  7.5  volts  above  the  9 volts.  For  power  conservation,

            the reader may connect a power switch in series with the battery.
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