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that  carry  the  difference- and  summing-frequency  terms  are  intermodulation

            distortion products or signals.
            And  in  superheterodyne  receivers,  the  IF  signal  from  the  mixer  has  a  difference
            frequency  such  as  (Fl - F2),  where  Fl is the frequency  of the  local  oscillator,  and
            F2 is the frequency of the input RF signal.
                       Distortion Can Be a Good Thing (for Mixing)

            We  have  seen  how  an  FET  with  an  approximate  square-law  characteristic  can  act

            as  a  linear  summer  and  as  a  mixer/multiplier.  This  square-law  characteristic
            generates  distortion  in  terms  of harmonic  and  intermodulation  distortion  products
            at the drain of the FET.
            FETs  are  used  as  mixers,  and  often  to  provide  good  mixing  action.  Typically  the
            local  oscillator's voltage (Le., combined with the RF signal)  is in  the amplitude level
            of volts peak to peak.  The reason  for this is that the FET is such  a linear device that

            huge amounts of input voltage are required to drive the FET into "usable" distortion
            that provides adequate levels of the IF signal.
                              Single-Bipolar-TranisistorDistortion

            Now  suppose  that  we  would  like  to  use  a  bipolar  transistor  for  mixing.  As
            mentioned  previously,  a  bipolar-transistor  amplifier  with  its  emitter  grounded
            AC-wise  has an exponential function:




                               I  -
                                ~
            where  VBE  is  the  total  voltage  across  the  base  emitter junction  of the  transistor,
            which  includes a DC bias voltage VBEQ  plus the AC signal voltage V sig • Thus


                                                                   +
                                                             I  .          i.
            The collector current can  be expressed equivalently as


                      (  , l~'"                                         v  ~/(!S!J
                                                                               I
                                                      s
            The  DC or quiescent collector current is just







            Figure  14-5  presents  an  example  of a common  emitter amplifier.  In the  figure,  a

            common  emitter amplifier with  J3  >  lOO,  the  DC  emitter current is  essentially equal
            to the DC collector current. Thus VE/R E = I cQ .
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