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05 overvoltages and insulation coordination

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425<br />

5.1.3.2. Load switching<br />

de-energizing loads<br />

inductive load<br />

single-phase circuit<br />

Let us consider the equivalent single-phase diagram in figure 5-25 with an ideal circuit-breaker<br />

CB which has a zero arc resistance the instant the contacts separate <strong>and</strong> which carries out<br />

interruption when the current crosses zero. Before operation of the circuit-breaker, between<br />

pointsA <strong>and</strong> B, there is a voltage drop due to the load current flowing through L s .<br />

At the instant of interruption, the voltage at B suddenly reaches the voltage at A <strong>and</strong> the<br />

capacitance C s is charged through L s . The energy exchanges between C s <strong>and</strong> L s make<br />

voltage oscillations at frequencies of 5 to 10 kHz occur.<br />

The voltage at<br />

C suddenly decreases to zero <strong>and</strong> the capacitance C p is then discharged<br />

through L . The energy exchanges between C p <strong>and</strong> L create voltage oscillations at<br />

frequencies going from 1 to 100 KHz.<br />

A<br />

I s<br />

B<br />

I D<br />

I 0<br />

CB<br />

C<br />

I L<br />

L s<br />

V A<br />

C s<br />

C p<br />

L<br />

L p<br />

L s : network inductance upstream of the circuit-breaker<br />

C s : network capacitance upstream of the circuit-breaker<br />

L : load inductance<br />

L p : stray inductance<br />

C p : network capacitance downstream of the circuit-breaker<br />

CB : circuit-breaker<br />

Figure 5-25: interruption in an inductive load network<br />

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Industrial electrical network design guide T & D 6 883 427/AE

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