2.2 Distance protection
65
7SA522 Manual
C53000-G1176-C155-3
2.2.1.2 Calculation of the Impedances                 
  A separate measuring system is provided for each of the six possible impedance loops 
L1-E, L2-E, L3-E, L1-L2, L2-L3, L3-L1. The phase-earth loops are evaluated when an 
earth fault detection is recognized and the phase current exceeds a settable minimum 
value 0LQLPXP,SK!. The phase-phase loops are evaluated when the phase current 
in both of the affected phases exceeds the minimum value 0LQLPXP,SK!.
A jump detector synchronizes all the calculations with the fault inception. If a further 
fault occurs during the evaluation, the new measured values are immediately used for 
the calculation. The fault evaluation is therefore always done with the measured 
values of the current fault condition.
Phase-Phase 
Loops
To calculate the phase-phase loop, for instance during a two-phase short circuit L1-L2 
(Figure 2-11), the loop equation is:
I
L1
 · Z
L
 – I
L2
 · Z
L
 = U
L1-E
 – U
L2-E
with
U
, I  the (complex) measured quantities and
Z
 = R + jX  the (complex) line impedance.
The line impedance is computed to be
Figure 2-11 Short-circuit of a phase-phase loop
The calculation of the phase-phase loop does not take place as long as one of the con-
cerned phases is switched off (during single-pole dead time), to avoid an incorrect 
measurement with the undefined measured values existing during this state. A state 
recognition (refer to section 2.20.1) provides the corresponding block signal. A logic 
block diagram of the phase-phase measuring system is shown in Figure 2-12.