19 January 2014

Arcing Ground (explained)

Arcing Ground Phenomenon

Already explained in previous blog arcing ground is a phenomenon which is observed in ungrounded 3 phase system. The voltage across this capacitance is phase voltage. During fault this voltage reduced to zero in faulted line where as in other phase increased by a factor of √3.
The arc between the faulty conductor and ground gets extinguished and restarts many times, this repeated initiation and extinction across the fault causes severe voltage oscillations of order nearly 3 to 4 times that of nominal voltage. Which damages the equipment insulation breakdown.


Above Diagram shows circuit diagram (a) and vector diagram (b) of a ungrounded system under normal condition:
Under normal condition the capacitance between lines are negligible compared to line to ground capacitance.
Here line to ground capacitance CR=CY=CB=C(say)* and voltages across capacitors are phase voltage i.e VRN,VYN and VBN.
So, capacitive current IR=IY=IB=Vph/Xc.The capacitive currents IR , IY and IB lead their respective phase voltages VRN, VYN and VBN by 90° as shown in the phasor diagram (b). The three capacitive currents are equal in magnitude and are displaced 120° from each other. Therefore, their phasor sum is zero, so no current flows to ground and the potential of neutral is the same as the ground potential. Therefore, ungrounded neutral system poses no problems under normal conditions.

Following diagram (c) and (d) shows the circuit and vector diagram of a ungrounded system with a fault in single line( line B) to ground fault at point F.
 
 
The voltage driving IR and IY through line R and Y are VBR and VBY. Here VBR and VBY are line voltages and IR and IY are essentially capacitive.
So, IR=IY=√3*Vph/Xc
The fault current IC in line B is vector sum of IR and IY,hence IC=IR+IY=3*Vph/Xc.

Conclusion:
  • The capacitive current in the two healthy phases increase to √3 times normal per phase capacitive current.
  • The capacitive fault current IC becomes 3 times the normal per phase capacitive current.
  • The potential of the faulty phase becomes equal to ground potential. However, the voltages of remaining healthy phases increased to √3 times of phase voltage i.e line voltage which is sufficient to start arcing ground and insulation breakdown of the equipment.

*
assuming transposed line

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