MV design guide - Schneider Electric
MV design guide - Schneider Electric
MV design guide - Schneider Electric
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Design rules<br />
Short-circuit currents<br />
The complexity in calculating<br />
the three-phase short-circuit current<br />
basically lies in determining the<br />
impedance value in the network<br />
upstream of the fault location.<br />
Example of a three-phase calculation<br />
Impedance method<br />
All the components of a network (supply network, transformer, alternator,<br />
motors, cables, bars, etc) are characterised by an impedance (Z)<br />
comprising a resistive component (R) and an inductive component (X) or<br />
so-called reactance. X, R and Z are expressed in ohms.<br />
c The relation between these different values is given by:<br />
(cf. example 1 opposite)<br />
Z = (R 2 + X 2 )<br />
Example 1:<br />
Network layout<br />
Tr1 Tr2<br />
c The method involves:<br />
v breaking down the network into sections<br />
v calculating the values of R and X for each component<br />
v calculating for the network:<br />
- the equivalent value of R or X<br />
- the equivalent value of impedance<br />
- the short-circuit current.<br />
c The three-phase short-circuit current is:<br />
A<br />
Equivalent layouts<br />
Zr<br />
Isc =<br />
U<br />
e • Zsc<br />
Za<br />
Zt1<br />
Zt2<br />
Isc : short-circuit current (in kA)<br />
U : phase to phase voltage at the point in question<br />
before the appearance of the fault, in kV.<br />
Zsc : short-circuit impedance (in ohms)<br />
Z = Zr + Zt1//Zt2<br />
Z = Zr + Zt1 • Zt2<br />
Zt1 + Zt2<br />
(cf. example 2 below)<br />
Za<br />
Zsc = Z//Za<br />
Zsc = Z • Za<br />
Z + Za<br />
Example 2:<br />
c Zsc = 0.72 ohm<br />
c U = 10 kV<br />
Isc =<br />
10<br />
= 21.38 kA<br />
e • 0,27<br />
<strong>Schneider</strong> <strong>Electric</strong><br />
Merlin Gerin <strong>MV</strong> <strong>design</strong> <strong>guide</strong><br />
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