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328     Fundamentals of Magnetic Thermonuclear Reactor Design



              TABLE 11.2 Parameters of Power Supplies for Toroidal Field
              Superconducting Coils

                                                  Tore              KSTAR
                               T-7      T-15      Supra    EAST     (Rep. of
              Parameters       (Russia)  (Russia)  (France)  (China)  Korea)
              Energy stored in coil   20  760     600      370      500
              magnetic field (MJ)
              Installed power of   0.2  0.4                0.34     1.2
              AC/DC converter
              (MVA)
              Maximum power    3.8      58        80       52       142
              at energy discharge
              (MW)
              Maximum current   6.3     5.3       1.4      16       40
              (kA)
              Maximum PS       40       75                 20       30
              voltage (V)
              Maximum          0.6      11        540 (26)  3.2     4
              total voltage at
              emergency energy
              discharge (kV)
              Voltage to ground at   0.3  1.5     1.7      1.6      6
              emergency energy
              discharge (kV)
              Time constant of   10     104       15       14.5     7
              emergency energy
              discharge (s)




            of time making it possible to essentially reduce power of the PS, namely, the
            AC/DC converter.  The latter provides current increase and decrease in the
            coils according to a given programme and its stabilisation at a prescribed level
            (Table 11.2).
               Coil protection at local superconductor-to-normal transition (quench) is, in
            fact, the main challenge in the superconducting coil PS system design. To pre-
            vent the normal phase propagation, which can potentially cause an accident, the
            stored energy has to be quickly removed from the coils.
               The energy discharge time is selected such that a fault coil section is not
            damaged. However, the shorter is the discharge time the higher the voltage is to
            be applied to the coil.
               The coil current can be quickly reduced by inserting a discharge resistor
            into the circuit (Fig. 11.3). As a rule, it is initially connected in series with the
            coil, but in a normal operating mode, it is bypassed by a circuit breaker (CB).
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