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20/660 Industrial Power Engineering and Applications  Handbook
        20.2  Analysis of  ungrounded and                = JIi2 + Ip" + 2. I; .I; . COS. 60"  (as  in  Section
              grounded systems                            15.4.3)

        This is related more to an HT system.
                                                         =    1;  (but this current may not be enough to trip
        20.2.1  Analysis of an ungrounded system
                                                          a protective relay)
        This is common to
                                                       The voltage across the healthy phases is now  fi times
          A three-phase three-wire, star connected isolated neutral   or 73%  more  than  the  phase  to  neutral  voltage  under
          system,                                      healthy conditions.
          A delta connected system, or                   Under certain line to ground impedance conditions,
          A three-phase four-wire, ungrounded  system.   when the ground circuit may also contain some inductive
                                                       reactance,  the  voltage  of  the  healthy  phases  may  rise
        An ungrounded a.c. system is more often subject to over-   further, much above the system voltage, due to resonance
        voltages. The reason is that even when the system is not   and ferro-resonance effects (see below). All this in turn
        connected to ground, it makes a ground connection through   may tend to swing the system to an unstable state. It may
        the  coupling  of  the  leakage ground  capacitances,  as   also cause arcing grounds* at the supporting insulators,
        illustrated in Figure 20.2. For all purposes these capaci-   leading to  voltage  surges, travelling in  both  directions
        tances may be regarded as equal and uniformly distributed,   along the line, and may be enough to cause damage to
        providing a balanced  system. In the event of  a ground   the line insulators and the terminal equipment.
        fault,  this circuit  is  closed  as  shown  and  a  capacitive   The magnitude of  overvoltage will  depend upon the
        current, I',,  flows back  to the healthy phases  via  these   actual inductive reactance introduced through the ground
        capacitances  Cg, Analysing  the  circuit  of  Figure 20.2,   circuit. The unintentional introduction of  an impedance
        the following may be derived:                  into the ground leakage capacitive circuit is generally a
                                                       result of a ground fault in the main equipment such as a
        If   C, = electrostatic  or  leakage  capacitance to  the   gcncrator, a transformer, power capacitors or an induction
                ground per phase, providing the return path to   motor  and when one or more  of  their  phase  windings
                the fault current Ig, in  the event of  a ground   forms a part of the ground circuit, as illustrated in Figure
                fault  on  the  system.  This  current  will  be   20.3.  Under such  conditions,  they  will  introduce  their
                capacitive in nature.                  own inductive, capacitive or resistive impedances or a
           Xcg = ground capacitive reactance per phase   combination of them into the ground circuit and alter the
                                                       parameters of the ground capacitive circuit. Figure 20.5
                                                       illustrates the system of Figure 20.2, drawn simply on a
                                                       singlc phase basis. The current through the ground circuit
        Under transient conditions, f becomes surge frequency,   will be zero when the system is healthy, the ground leakage
        fs and                                         capacitances finding no return path (Figure 20.6). It is
                                                       not necessary that the equipment itself should develop a
                       1
        Xc, becomes,                                   ground fault and then only its impedance will be inducted
                    2xfs . C,                          into  the  ground  circuit.  It  may  be  introduced  into the
                      1                                circuit  even  when  there  is  a  line  or  a  system  ground
        where fs =                                     fault, as  illustrated  in  Figure 20.4.  The ground circuit
                  27c J   l                            may give rise to dangerous voltages in the healthy phases,
        L being the inductance of the circuit.         as analysed below.
        If    I, = ground fault current
             V, = ground potential, which is the same as zero   (1) When the external impedance is a resistance
                 sequence voltage or residual voltage   or a capacitive reactance
             Vt = line voltage and
             Vp = phase voltage                        Referring to Figure 20.5, if  Z; is the external impedance
                                                       introduced into the natural leakage ground circuit, as a
        then on a ground fault, say, in phase R, the voltage across   consequence of a ground fault, as shown in Figures 20.3
        this phase will reduce to zero, while the ground potential
        across the healthy phases will rise to V, from a zero level
        earlier. It will  cause  a  fault current  Zi, in  the healthy   * Arcing grounds: This occurs during a temporary ground fault on
        phases  also,  through  the  ground  leakage  capacitances   an ungrounded HT system. It causes an arc between the line conductor
        such that  I:  = VI/X,,  (assuming the ground circuit has   and the ground, which may be direct or through the flashover of the
                                                       line insulators, due to overvoltage. The ground leakage capacitors
        no other impedance) and the ground fault current through   that may be considered as charged with the line voltage are discharged
        the grounded circuit,                          to  the  ground  on developing  a ground  fault. The supply  voltage
            _-                                         would charge them again and  so the process  will repeat  until the
        I,  =  I,  + I,                                fault exists. The repeated discharges and charges of ground capacitors
                                                       during the fault produce arcs and are termed arcing grounds, giving
          = r,' + I,' (both phasors being 60" apart)   rise to voltage surges.
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