A commutation and breaking method for a DC vacuum switch commutation and breaking device
A vacuum switch and breaking device technology, applied in the direction of emergency power supply protection, etc., can solve the problems such as the difficulty in realizing the bidirectional symmetrical breaking function of the vacuum switch S, and achieve the effects of convenient bidirectional symmetrical breaking, reduced volume, and reduced current change rate
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Embodiment 1
[0027] When the DC current of the main circuit of the system flows from terminal J1 to terminal J2, during the commutation breaking process, refer to Figure 4 and Figure 5 As shown, the vacuum switch S first breaks off to generate an arc; then the auxiliary switches S1 and S4 are turned on, and the pre-charge capacitor C discharges through the loop formed by the inductor L-auxiliary switch S4-vacuum switch S-auxiliary switch S1 to generate pulse current i C , then the effective commutation current is i com = i C , forcing the current i in the vacuum switch S S Decrease rapidly; at current i S At a certain moment Δt1 near zero, the auxiliary switch S2 is turned on, and the pulse current (discharge current) i C Part of the current i in S2 Flowing through the auxiliary switch S2, the effective commutation current is reduced to i com = i C -i S2 , so as to greatly slow down the current change process near the zero-crossing of the vacuum switch S current; when the vacuum ...
Embodiment 2
[0029] When the DC current of the main circuit of the system flows from terminal J2 to terminal J1, during the commutation breaking process, refer to Figure 6 and Figure 7 As shown, after the vacuum switch S is broken to generate an arc, the auxiliary switches S2 and S3 are turned on, and the precharge capacitor C discharges through the loop formed by the inductance L-auxiliary switch S3-vacuum switch S-auxiliary switch S2 to generate a pulse current i C , then the effective commutation current is i com = i C , forcing the current i in the vacuum switch S S Decrease rapidly; at current i S At a certain moment Δt1 near zero, the auxiliary switch S1 is turned on, and the pulse current (discharge current) i C Part of the current i in S1Flowing through the auxiliary switch S1, the effective commutation current is reduced to i com = i C -i S1 , so as to greatly slow down the current change process before the current of the vacuum switch S crosses zero; when the current of...
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