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         same as that of the impedance of a motor during a start,   Stator minimum heat
        in  a  balanced  supply  system. Thus,  the  current  effect
        during normal  running of a  negative  sequence voltage   This occurs in the other two windings, which are  120"
        will be the same as that of the starting current effect on   phase apart (Figure 12.5). Hence
        a balanced supply system.
          The  effect  of  voltage  unbalance  is,  therefore,  more   I,,(min.)  = $I:  + I:  + 21,  x I, cos 60"
        pronounced than the percentage of unbalance itself. For   = J7-c
         instance, a voltage unbalance of 3% may cause a current
        unbalance of 18-30%,  which is detrimental to the life of
         the motor.  The effective current in the stator windings   and the minimum heat generated,
         would depend upon the relative positions of the positive
         and  the  negative  sequence components.  In  one of  the   H,, (min.) = ( I,'  + 1,2  + I, x I,
         windings they may be in phase, producing the maximum
         current and the associated heating effect, and in the other   (Figure 12.3, curve 2)   (12.5)
         two  they  may  be  120" apart.  In  Figure  12.5 we have
         drawn the maximum and the minimum effective currents   Example 12.3
         which  the  stator  windings  may  experience  on  an  un-   The minimum heat generated in the above case
         balanced supply system.                       Heq (min.) = (1'  + 0.4'  + 1 x 0.4)
                                                       or      = (1 + 0.16 + 0.4)
          Stator maximum heat
                                                       i.e.  1.56 or  156%
         This  occurs  when  the positive  and  negative  sequence
         components fall in phase in which case the equivalent   Stator average heat
         stator current will become
                   -   -                               In practice the temperature attained by the stator windings
         I,,  (max.) = I, + I,
                                                       will  be  significantly below  the  maximum  or even  the
         and the maximum heat generated, Heq(max.) ..(I,  + IJ2   minimum heats as determined above due to the heat sink
         (Figure 12.3, curve  1)                       effect. The heat will  flow from the hotter phase to the
                                                       cooler phasedarea (see curve 3 of Figure 12.3). But for
         or  H,,(max.)   0~  (I,? + I,'  + 21,  x I, )   (12.4)   protection of the motor windings against negative sequence
                                                       components, the average heat curve is of no relevance,
         Example 12.2                                  for it will take a considerable time for the heat to stabilize
         Consider  a  negative sequence  component  of  40%  of  the   at this curve, and much more than the thermal withstand
         rated current. Then the maximum heat generated as in equation   capacity of the winding most affected.
         (1  2.4)                                        It is therefore essential to provide adequate protection
         Heq (max.) = (1'  + 0.4' + 2 x  1 x 0.4)       for the  motor to disconnect it  from the mains quickly
                                                       before any damage is caused to the most affected winding.
         or      = (1 + 0.16 + 0.8)                    The protection is based on the maximum heat that may
         i.e.  1.96 or 196%                             be  generated  in  the  motor  windings  in  the  event  of  a
                                                        negative sequence component in the system.

                                                         Magnitudes of negative sequence components
                                                       for protection
                                                        The additional  heat  generated  by  a  negative  sequence
                                                        component may vary from six to ten times the theoretical
                                                        heat  produced  by  that  amount  of  a  positive  sequence
                                                        component, as analysed above. It is therefore more relevant
                                                        to consider a factor of 6 to represent the effect of such a
                                                        component. The heat generated can be rewritten as

                                                        He,  = (I,? +6Z,')                    (12.6)
                                                        and the current on unbalance,



                                                        The factor 6 is a design parameter for all future reference.
                                                        In  fact, this empirical factor has been established over
                                                        many years of experience and field data collected on the
                                                        behaviour  and  performance  of  a  motor  in  such  an
         Figure 12.5  Equivalent stator currents during unbalanced voltage   unfavourable operating condition.
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