Limitation in thermal magnetic protection devices

Principe

NoteConsider the minimum circuit opposite, where:

  • Ua : arc voltage created when the contacts of circuit-breaker A open

  • Zs : load, point of appearance of fault

  • Zcc : short-circuit impedance

  • i : current flowing in the mesh

  • e : emf when the short-circuit appears

NoteFor a full short-circuit, we have the following equations:

  • E =R.i + L.di/dt + Ua, where E is the source voltage.

  • R.i can be considered to be negligible compared with L.di/dt:

  • e = L.di/dt + Ua , thus limitation achieved more easily and quick decrease of Ic

When di/dt = 0, current i reaches its maximum value (= peak value), i.e. for Ua = e.

Fundamental

See the interpretation in the graphs opposite, where ts is the time when voltage Ua appears, i.e. in the circuit-breaker case, when the contacts open.

  • In short, limitation will be correct when: Ua max. = UM > EM (of source)

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