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with  a larger valued  inductor CL3)  and  load  resistor  CRS).  Thus the gain  of the Q2

            amplifier at its collector is about 30 or 40.
            It should  be  noted  that  there  are  resistors  connected  in  parallel  to  the  load
            inductors.  This  is  to ensure that the  amplifiers do  not oscillate  by  limiting the gain
            at  high  frequencies.  An  inductor's  impedance  increases  with  frequency.  For
            example,  removing  the  20-ko  resistor  across  L2  will  result  in  an  oscillating  circuit
            instead of an amplifying circuit.

            With  amplifiers Ql and  Q2, the total gain  is  about 300 to 400.  To  demodulate the
            amplified  AM  signal,  a  germanium  diode  is  used  as  an  envelope  detector  with  a
            peak  hold  capacitor  C7.  Note  that  the  peak  hold  capacitor  provides  a
            larger-amplitude  audio  signal  than  without  C7.  Resistor  R6  allows  for  a discharge
            path  to  C7  so  that the  audio  signal  is  demodulated  without gross  distortion  when

            the  AM  signal's  envelope  is  decreasing.  Without a discharge  resistor  on  the  peak
            hold  capacitor,  the  demodulated  signall will  be  "stuck" at a voltage  related  to  the
            peak  of the  AM  signal.  DC  blocking  capacitor  C8  then  is  connected  to  a  crystal
            earphone  for  listening.  Note:  One  lead  of the  crystal  earphone  is  connected  to
            ground.

                Variation of the Design (Alternate Design of the TRF
                                                       Radio)

            A variant of this  design  was  tried  with  a  loop  antenna  with  antenna  transformer.
            Because there  is  less  RF signal  from  this combination,  loop antenna/transformer as
            compared  to  a  ferrite  antenna  coil,  an  extra  stage  of amplification  was  added

            (Figure 5-2).
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