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Page Title: Radiation and Induction Losses
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ELECTROMAGNETIC FIELDS
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Electronics Technician Volume 07-Antennas and Wave Propagation
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Ac Applied to a Transmission Line

Another  type  of  copper  loss  is  due  to  SKIN EFFECT.  When  dc  flows  through  a  conductor,  the movement  of  electrons  through  the  conductor’s  cross section is uniform, The situation is somewhat different when  ac  is  applied.  The  expanding  and  collapsing fields  about  each  electron  encircle  other  electrons. This phenomenon, called SELF INDUCTION, retards the  movement  of  the  encircled  electrons.  The  flux density at the center is so great that electron movement at  this  point  is  reduced.  As  frequency  is  increased, the  opposition  to  the  flow  of  current  in  the  center  of the  wire  increases.  Current  in  the  center  of  the  wire becomes  smaller  and  most  of  the  electron  flow  is  on the  wire  surface.  When  the  frequency  applied  is  100 megahertz  or  higher,  the  electron  movement  in  the center  is  so  small  that  the  center  of  the  wire  could be  removed  without  any  noticeable  effect  on  current. You  should  be  able  to  see  that  the  effective  cross- sectional  area  decreases  as  the  frequency  increases. Since   resistance   is   inversely   proportional   to   the cross-sectional area, the resistance will increase as the frequency   is   increased. Also,  since  power  loss increases  as  resistance  increases,  power  losses  increase with  an  increase  in  frequency  because  of  skin  effect. Copper  losses  can  be  minimized  and  conductivity increased in an rf line by plating the line with silver. Since  silver  is  a  better  conductor  than  copper,  most of  the  current  will  flow  through  the  silver  layer.  The tubing then serves primarily as a mechanical support. Dielectric Losses DIELECTRIC  LOSSES  result  from  the  heating effect  on  the  dielectric  material  between  the  conductors. Power from the source is used in heating the dielectric. The heat produced is dissipated into the surrounding medium. When  there  is  no  potential  difference between  two  conductors,  the  atoms  in  the  dielectric material  between  them  are  normal  and  the  orbits  of the  electrons  are  circular.  When  there  is  a  potential difference  between  two  conductors,  the  orbits  of  the electrons  change.  The  excessive  negative  charge  on one conductor repels electrons on the dielectric toward the  positive  conductor  and  thus  distorts  the  orbits  of the  electrons.  A  change  in  the  path  of  electrons requires  more  energy,  introducing  a  power  loss. The  atomic  structure  of  rubber  is  more  difficult to  distort  than  the  structure  of  some  other  dielectric materials. The atoms of materials, such as polyethyl- ene,  distort  easily.  Therefore,  polyethylene  is  often used  as  a  dielectric  because  less  power  is  consumed when  its  electron  orbits  are  distorted. Radiation and Induction Losses RADIAION   and   INDUCTION   LOSSES   are similar in that both are caused by the fields surround- ing  the  conductors.  Induction  losses  occur  when  the electromagnetic  field  about  a  conductor  cuts  through any  nearby  metallic  object  and  a  current  is  induced in that object. As a result, power is dissipated in the object  and  is  lost. Radiation  losses  occur  because  some  magnetic  lines of  force  about  a  conductor  do  not  return  to  the conductor  when  the  cycle  alternates.  These  lines  of force  are  projected  into  space  as  radiation,  and  this results  in  power  losses.    That  is,  power  is  supplied by  the  source,  but  is  not  available  to  the  load. VOLTAGE   CHANGE In  an  electric  circuit,  energy  is  stored  in  electric and  magnetic  fields.  These  fields  must  be  brought to the load to transmit that energy. At the load, energy contained in the fields is converted to the desired form of  energy. Transmission of Energy When the load is connected directly to the source of  energy,  or  when  the  transmission  line  is  short, problems concerning current and voltage can be solved by  applying  Ohm’s  law.  When  the  transmission  line becomes  long  enough  so  the  time  difference  between a  change  occurring  at  the  generator  and  a  change appearing  at  the  load  becomes  appreciable,  analysis of  the  transmission  line  becomes  important. Dc Applied to a Transmission Line In  figure  3-7,  a  battery  is  connected  through  a relatively  long  two-wire  transmission  line  to  a  load at  the  far  end  of  the  line.  At  the  instant  the  switch 3-4

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