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         it such as a  switching device to a  cable, a cable to an   1       2       3
         overhead  line or a transformer  and an induction motor
         etc, then the frequency of  oscillations will continue to
         alter after every junction. At each junction the travelling
         wave  will  encounter  a  wave  reflection  and  add  more
         impedance in its circuit, as it will propagate ahead. After
         every reflection,  the circuit  parameters  will  change  as
         will  the  frequency  of  uscillations.  Thus,  a  number  of
          oscillatory frequencies may exist in the system at a time,
          leading to a more complex phenomenon  and making it
          difficult  to  accurately  determine the  effective  surge
          frequency  of  the  system  and the  r.r.r.v.  By  the  use  of
          oscillograms  such  as  that  shown  in  Figure  17.5,  it  is
          possible to determine such complex quantities.
           The  higher  the  frequency  of  the  transient  recovery
          voltage (TRV), the steeper will be the slope of the TRV
          (Figure 17.6), Le. the higher will be the r.r.r.v. The r.r.r.v.
          is  a measure  of  severity  of  the TRV  that  the terminal
          equipment and the devices may have to endure.                    Time Ips)
          17.6.4  Surge impedance                           For same peak voltage 'V,'
                                                            tl  <  ti  <  f;  and
          The  shape  and  characteristics  of  a  surge  wave  are   fSl  > f*z  '
                                                                   fs3
          influenced  by  the  circuit  parameters,  Le.  the  leakage   VI   vt  vt
          inductance L of the interconnecting cables and the current-   and r.r.r.v =  - - -
                                                                          >
                                                                        t;
                                                                           t;
                                                                     tl
          carrying components of the equipment through which it
                                                        Figure 17.6  The variation of r.r.r.v. with the front time  (tl  0~  2)
                  15
                                                        travels and the leakage capacitance C of such cables and
                  10                                    the  motor  dielectric  lumped  capacitance  etc.  (Section
                                                        9.6.1). The relation between L and C that will determine
                                                        the shape of the travelling wave is known as the surge or
                                                        natural  impedance 2, of the system and is expressed as:
                                                         z, = Et2
                W
                N                                                                              (17.2)
                                                        where
                              Time -
                                                         L = circuit leakage inductance in henry (H), and
                  20                                    C = circuit lumped leakage capacitance in farad (F).
                            0  0.5 1.0  1.5  2.0  2.5  3.0
                  (a) Without surge arrester maximum peak to peak   Influence of surge impedance  on terminal
                                                        equipment
                    voltage = 26 kV
                                                        These values (L and C) help to determine the likely surge
                   15                                   voltages that may develop during a switching operation
                                                        while using different interrupting devices. For accurate
                                                        analysis, it is advisable to obtain these values from their
                                                        manufacturers.  Slamecka  (1 980)  and  others  have  also
                                                        established such curves and have provided them in the
               r
                                                        form  of  nomograms  for  easy  identification  of  this
                                                        parameter, as reproduced in Figures 17.7(a) and (b). The
                                                         surge impedance Z, varies with variations in the design
                                                        parameters,  hence from manufacturer  to  manufacturer.
                   10                                   These curves have therefore been provided in the form
                                                        of bands. To account for likely variations in the design
                   15
                        0   0.5  1.0  1.5  2.0  2.5  3.0   parameters  by  the  different  manufacturers  one can,  at
                               Time                     best,  obtain  an  average value  of  the  surge  impedance
                                                         from these curves for a particular machine, as illustrated
                   (b)  With surge arrester maximum peak to peak   for a 500 h.p.  (= 500 kVA) motor.  But for an accurate
                      voltage = 13.5 kV
                                                         value, it must be obtained from the machine manufacturer
          Figure 17.5  Oscillograms showing the effectiveness of a surge   alone, as shown in Figure 17.7(c), for curves produced
          arrester  on a 6.6 kV motor                    by  Siemens for their motors.
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