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268  Electrical equipment

                 current-carrying  conductor  in  a  magnetic  field  produces  the  motor
                 effect  which turns the  rotor.  The  motor  speed  builds up  to a value just
                 less than  the  speed  of rotation  of the  magnetic field.
                   The  motor  speed  depends  upon  the e.m.f. induced  in the  rotor  and
                 this depends  upon  the difference in speed  between the conductors and
                 the magnetic field. If the  load is increased  the rotor  slows down slightly,
                 causing an increase  in induced  e.m.f. and  thus a greater torque  to deal
                 with  the  increased  load.  The  motor  is almost constant  speed  over  all
                 values of  load.  It  will  start against about  two times full  load  torque  but
                 draws a starting current  of about six times the normal full  load current.
                 The  starting  current  can  be  reduced  by  having  a  double  cage
                 arrangement on the rotor. Two separated  cages are provided, one below
                 the  other  in  the  rotor.  When  starting,  the  outer  high-resistance cage
                 carries  almost  all  the  rotor  current.  As  the  motor  accelerates  the
                 low-resistance inner winding takes more and more of the current until it
                 carries the  majority.
                   A  number  of  different  fixed  speeds  are  possible  by  pole changing.
                 The  speed  of an  induction motor  is proportional  to  frequency divided
                 by the numbers of pairs of poles. If therefore a switch is provided which
                 can  alter  the  numbers  of  pairs  of  poles,  then various fixed speeds  are
                 possible.  The  number  of  poles  affects  the  starting  characteristics such
                 that the  more  poles the less the starting torque  to full  load  torque  ratio.
                   Only  the  induction  type of  a.c.  motor  has  been  described,  since it is
                 almost  exclusively  used  in  maritime work.  Synchronous  motors  are
                 another  type which have been  used for electrical propulsion systems but
                 not auxiliary drives.
                   A  number  of  different  arrangements  can  be  used  for  starting  an
                 induction  motor.  These  include  direct  on-line,  star  delta,  auto
                 transformer  and  stator  resistance. Direct on-line starting is usual where
                 the  distribution  system  can  accept  the  starting  current.  Where  a  slow
                 moving high inertia load is involved the starting time must be  considered
                 because  of  the  heating  effect  of  the  starting  current.  The  star  delta
                 starter  connects  the  stator  windings  first  in  star  and  when  running
                 changes over  to delta.  The  star connection results in about half of  the
                 line  voltage being applied  to  each  phase  with  therefore  a reduction  in
                 starting current.  The  starting torque is also reduced  to about one-third
                 of  its direct  on  line value. A rapid  change-over  to  delta  is required  at
                 about  75%  of  full  load  speed  when  the  motor  will  draw  about
                 three-and-a-half times its full  load current. The auto transformer starter
                 is  used  only  for  large  motors.  It  uses  tappings  from  a  transformer  to
                 provide,  for  example,  40%,  60%  and  75% of  normal  voltage  (Figure
                 14.12).  The  motor  is started  on  one  of  the  tappings  and  then  quickly
                 switched to full  voltage at about 75% full  speed.  The  tapping chosen  will
                 depend  upon  the  starting torque  required  with  a  60% tapping  giving
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