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Page Title: Electron Resonance
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MAGNETRON   OPERATION

netron  so  that  the  magnetic  field  is  parallel  with  the axis   of   the   cathode.   The   cathode   is   mounted   in   the center   of   the   interaction   space.   The   direction   of   an electric   field   is   from   the   positive   electrode   to   the negative    electrode. The  law  governing  the  motion  of  an  electron  in  an electric   (E)   field   states   that   the   force   exerted   by   an electric  field  on  an  electron  is  proportional  to  the strength  of  the  field.  Electrons  tend  to  move  from  a point  of  negative  potential  toward  a  positive  potential. In  other  words,  electrons  tend  to  move  against  the  E field.  When  an  electron  is  being  accelerated  by  an  E field,  energy  is  taken  from  the  field  by  the  electrons. The  law  of  motion  of  an  electron  in  a  magnetic (H)  field  states  that  the  force  exerted  on  an  electron  in a  magnetic  field  is  at  right  angles  to  both  the  field  and the  path  of  the  electron.  The  direction  of  the  force  is such  that  the  electron  trajectories  are  clockwise  when viewed  in  the  direction  of  the  magnetic  field. Magnetron  oscillators  are  divided  into  two  classes: negative   resistance   and   electron   resonance. .   Negative   Resistance:   A  negative  resistance magnetron   oscillator   operates   by   a   static   negative resistance  between  its  electrodes  and  has  a  frequency equal  to  the  natural  period  of  the  tuned  circuit  con- nected  to  the  tube.  The  split-anode  negative  resistance magnetron   is   a   variation   of   the   basic   magnetron, which  operates  at  a  higher  frequency  and  is  capable  of more   output. .   Electron  Resonance:   An   electron   resonance magnetron   oscillator   operates   by   the   electron   transit- time   characteristics   of   an   electron   tube   (the   time   it takes  electrons  to  travel  from  the  cathode  to  the  plate). It  is  capable  of  generating  very  large  peak-power  out- puts  at  frequencies  in  the  thousands  of  megahertz.  The electron  resonance  magnetron  is  most  widely  used  for microwave   frequencies. Modern   designs   have   a reasonably  high  efficiency  and  relatively  high  output. However,  one  disadvantage  of  the  electron  resonance magnetron  is  that  its  average  power  is  limited  by  the cathode   emission.   Furthermore,   the   peak   power   is limited  by  the  maximum  voltage  that  it  can  withstand without    damage. The  operation,  coupling  methods,  tuning,  and seasoning   of   magnetrons   are   discussed   in   the   fol- lowing  subsections.  Since  this  information  is  general in   nature,   the   recommended   times   and   PMS   proce- dures   in   equipment   technical   manuals   should   be followed   when   baking-in   a   specific   type   of   magne- tron.  Figure  2-7  shows  a  magnetron. Figure   2-7.—Magnetron. 2-10

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