Siemens SIPROTEC 7UM62 Manual page 129

Measuring Principle
The 2 possible implementations of the earth fault differential protection differ only in their method of determining
the zero sequence current. This is shown in the following picture. This figure also shows the definition of the
current direction. The general definition is: Reference arrows run in positive direction to the protected object.
Figure 2-48
In both measuring principles, there is a vector addition of the phase currents on the line side (always side 1 in
the 7UM62), which yields the zero sequence current. The rule of calculation for side 1 is:
3I = I + I
01 L1S1
For the second zero sequence current, two methods of determination are possible:
On the one hand it is measured directly as the starpoint current at input I
the zero sequence current from the CTs on the starpoint side (always side 2 in the 7UM62). The pertinent for-
mulas are:
3I = I = I
02 St EE2
or
3I = I + I
02 L1S2
When an earth fault occurs in the protected zone, there is always a starpoint current I
current flowing through the CTs of side 2 (3I
be an earthing current (3I
definition of the current direction, however, the zero sequence current 3I
starpoint current.
When an earth fault occurs outside the protected zone (see next picture, fault location 2), there is also a star-
point current I
flowing through the CTs of side 1 (3I
surement locations. As the current direction flowing into the protected object is defined as positive, the zero
sequence current flowing on side 1 (3I
zero phase current of side 2 (3I
SIPROTEC, 7UM62, Manual
C53000-G1176-C149-7, Release date 03.2010
Connection scheme and definition of current vectors
+ I
L2S1 L3S1
+ I
L2S2 L3S2
) flowing through the CTs of side 1 to the fault location (dashed arrow). Due to the
01
or zero sequence current flowing through the CTs of side 2 (3I
St
). The zero sequence current must be the same at all three possible mea-
01
01
).
02
2.15 Earth Current Differential Protection (ANSI 87GN,TN)
). Depending on the network earthing conditions, there may also
02
) is in phase opposition to the starpoint current I
(I = I ). Method 2 is to calculate
EE2 St EE2
or zero sequence
St
is more or less in phase with the
01
) and a zero sequence current
02
or to the computed
St
Functions
129