Patent Number: 046684646
Section: claims

1. A method of maintaining three-dimensional MHD equilibrium of a plasma contained in a helical axis stellarator said stellarator having a set of primary coils, said method comprising the steps of: providing a current through a resonant coil system about said stellarator, said resonant coil system having a configuration such that said current therethrough generates a magnetic field cancelling the resonant magnetic field, B.sub.1, produced by currents driven by the plasma pressure at any given flux surface resonating with the rotational transform, .chi., of another flux surface in the plasma; and  varying said current as a function of .beta., where .beta.=2p.sub.o /B.sub.o 2, p.sub.o is the average plasma pressure, and B.sub.o is the average stellarator magnetic field produced by said primary coils.  a helical resonant coil system about said stellarator, said resonant coil system having a configuration such that current therethrough generates a magnetic field cancelling the resonant magnetic field, B.sub.1, produced by currents driven by the plasma pressure on any given flux surface resonating with the rotational transform, x=n/m, of another flux surface in the plasma, where m is the number of periods of said helical resonant coil and n is the number of turns of said helical resonant coil carrying current in the same direction; and  means for varying said current as a function of .beta., where .beta.=2p.sub.0 /B.sub.o.sup.2, p.sub.o is the average plasma pressure, and B.sub.o is the average magnetic field produced by the stellarator primary coils. 2. The method of claim 1 wherein said current is varied such that .beta. satisfies the relationship: ##EQU7## at rational surface .rho..sub.o and where m is the number of period of said coil and n is the number of turns of said coil carrying current in the same direction, L is the length of the stellarator axis, a is the circularized plamsa radius, .delta..sub.nm are the Fourier amplitudes of the Jacobian of the stellarator magnetic field, and .rho., .theta., .phi. ar helical coordinates. 3. The method of claim 2 wherein m=3, n=2 and wherein said current is varied such that .beta. satisfies the relationship: ##EQU8## .chi.=n/m and .DELTA..chi. is the change in .chi. across minor radius a. 4. In a helical axis stellarator having primary coils, an apparatus for maintaining three-dimensional MHD equilibrium in a plasma contained in said helical axis stellarator, said apparatus comprising: 5. The apparatus of claim 4 wherein said means for varying said current is operable to vary the current such that .beta. satisfies the relationship ##EQU9## at rational surface .rho..sub.o with .chi.=n/m and where L is the length of the stellarator axis, a is the circularized plasma radius, .delta..sub.nm are the Fourier amplitudes o the Jacobian of the stellarator magnetic field, and .rho., .theta., .phi. are helical coordinates. 6. The apparatus of claim 5 wherein said stellarator has three periods and wherein said means for varying said current is operable to vary the current such that B satisfies the relationship ##EQU10## where .DELTA..chi. is the change in .chi. across minor radius a. 7. The apparatus of claim 6 wherein the magnitude of the current in said resonant helical coil is about 1% of the magnitude of the current in said stellarator primary coils.