are given in Tables 6.3 and 6.4. the first table has lower than nominal sector capacitor voltage (closer to the values used in preliminary testing of Mass Driver Two) and a current lower than what could be obtained operating at 800V. The second table has nominal sector capacitor voltage but a higher bucket coil current using the new capacitor bank. This last table shows that the ohmic bucket design can easily meet the nominal 500g1s design spec. Theoretical performance for the ohmic bucket (α= 0.63) at 300V on the sector capacitor for different bucket coil currents is shown in Fig. 6.4. Theoretical performance for the ohmic bucket (α = 0.63) with bucket coil current at 33,600 amp turns for different sector capacitor voltages is shown in Fig. 6.5. The superconducting bucket performance was calculated the same as the ohmic bucket except that the mass and current were higher. Theoretical performance of the superconducting bucket (a= 0.514) at nominal sector capacitor voltage and bucket coil current at 42,750 amp turns is shown in Table 6.5. The same superconducting bucket but operating with a bucket coil current of 80,000 amp turns is shown in Table 6.6. All previous performance calculations were done for the accelerator, now the performance of the decelerator will be presented. The theoretical performance of the decelerator operating at nominal sector capacitor voltage and with the a = 0.514 ohmic bucket at 45,000 amp turns is given Table 6.7.
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