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Extra resources for Electronuclear Ion Fusion In An Ion Cyclotron Resonance Reactor patent info
Since the ions are resonantly accelerated, 3He+ introduced on axis will not be accelerated. 10 Rather, it will remain trapped on axis, passing repeatedly into the ionizer until becoming doubly ionized, where tqxm it will be accelerated. Ion acceleration times and trapping lifetimes can be made long enough to allow the reactor of the present invention to be operated in a pulsed mode providing additional flexibility for separately optimizing trapping potentials and field shims for the acceleration 15 and interaction phases.
Q w m’ / \ Y.
Since the triton spends most of its life near radius R, the effect of this limitation is minimized if the RF frequency is tuned to the value given by Eq. (25) evaluated at r = R. 02R, this frequency is shifted by less than 1 ppm/volt in a 5 T field. Near r = rC, the shift can exceed several hundred ppm unless V, is limited to a few volts. This off-resonance effect can be eliminated by using axial field shims 64 (Figure 5A) for 10 tailoring the magnetic field and counterbalancing the logarithmic potential.