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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 />

17

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