2 Functions
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7SA522 Manual
C53000-G1176-C155-3
Figure 2-12 Logic of the phase-phase measuring system
Phase-Earth Loops For the calculation of the phase-earth loop, for example during a L3–E short-circuit 
(Figure 2-13) it must be noted that the impedance of the earth return path does not 
correspond to the impedance of the phase. In the loop equation
I
L3
 · Z
L
 – I
E
 · Z
E
 = U
L3-E
 Z
E
 is replaced by (Z
E
/Z
L
) · Z
L
 yielding:
From this the line impedance can be extracted
Figure 2-13 Short-circuit of a phase-earth loop
The factor Z
E
/Z
L
 solely depends on the line parameters and not on the fault distance.
The evaluation of the phase-earth loop does not take place as long as the affected 
phase is switched off (during single-pole dead time), to avoid an incorrect measure-
ment with the undefined measured values existing in this state. A state recognition 
provides the corresponding block signal. A logic block diagram of the phase-earth 
measuring system is shown in Figure 2-14.