Figure 85: Phasors For A Phase C Earth Fault In A Petersen Coil Earthed System; Figure 86: Zero Sequence Network Showing Residual Currents - GE MiCOM P40 Agile Technical Manual

Single breaker current differential (with distance)
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P543i/P545i
Assuming that no resistance is present in X
below:
I
H3
I
A
L
I
H2
I
H1
I
B1
I
A1
N
C
a) Capacitive and inductive currents
V00633

Figure 85: Phasors for a phase C earth fault in a Petersen Coil earthed system

It can be seen that:
The voltage in the faulty phase reduces to almost 0V
The healthy phases raise their phase to earth voltages by a factor of Ö3
The triangle of voltages remains balanced
The charging currents lead the voltages by 90°
Using a core-balance current transformer (CBCT), the current imbalances on the healthy feeders can be measured.
They correspond to simple vector addition of I
by exactly 90º.
The magnitude of the residual current I
the faulted feeder, the residual current is equal to I
shown in the following figure:
I
L
3X
-V
L
0
V00640

Figure 86: Zero sequence network showing residual currents

P54x1i-TM-EN-1
or X
, the resulting phasor diagrams will be as shown in the figure
L
C
3V
0
B
and I
A1
is equal to three times the steady-state charging current per phase. On
R1
- I
L
I
I
OF
ROF
I
ROH
I
ROH
IH
IH
IH
3
2
1
X
CO
I
= I
R1
H1
I
b1
I
a1
V
= -3V
res
o
b) Unfaulted line
, I
and I
, I
and I
B1
A2
B2
A3
B3
- I
(C). This is shown in the zero sequence network
H1
H2
Faulty feeder
Healthy feeders
Chapter 7 - Distance Protection
I
L
-I
H1
-I
H2
I
I
R3
R3
V
= -3V
res
o
c) Faulted line
, and they lag the residual voltage
I
= Residual current on faulted feeder
ROF
I
= Residual current on healthy feeder
ROH
I
= I
– I
– I
– I
OF
L
H1
H2
H3
I
= I
+ I
ROF
H3
OF
so:
I
= I
– I
– I
ROF
L
H1
H2
= I
+ I
F
H3
= I
- I
- I
L
H1
H2
181

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