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After assembly in the cryostat, both magnets reached their conductor-limited quench current.
The quench current (240 A at 4.2 K) was equal to that reached in the pool boiling LHe cryostat.
Current sharing was observed between two modules in the 20 kA current lead and the quench current was evaluated to about 30 kA at the design conditions.
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In this paper, we investigated the quenching current and the fault current limiting characteristics in accordance with the variations of designed parameters.
R1 quenches the current flow by lowering the voltage across the APD close to (V_{text{br}}) [38].
The EM loads during plasma disruptions are mainly produced by: (1) toroidal flux variation (TFV) during the thermal quench (TQ) and current quench (CQ); (2) halo currents (HC); and (3) poloidal flux variation (PFV) during TQ and CQ phase.
Both the poloidal and toroidal field variations due to the plasma movement and to the current quench are implemented.
The analysed transients include: eddy currents induced by a variation of all the magnetic field components, during both the thermal and the current quench phases and halo currents flowing from the plasma to the vessel during vertical displacement events (VDEs).
DINA analysis shows that although the ex-vessel VS control modifies radial field, it does not affect plasma motion and current quench behavior including halo current generation because the vacuum vessel shields the field created by the ex-vessel coils.
Eddy currents and related EM loads are calculated considering a VDE-up provided by CarMa0NL code with a 74 ms current quench time.
Since the unavailability of the details of the plasma in CFETR, when disruptions happen, the condition where a linear current quench of main disruption occurs was assumed.
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