AAWSAP DIRD, Aneutronic Fusion Propulsion II, November 2010
DOW-UAP-D146 · page 11 of 36
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UNCLASSIFIED/ /FOR. OFFICIAL t:191!!! OHL¥ magnetic mirror pole regions serve as a magnetic mirror or bottle that traps and reflects charged particles - the particles gain energy Figure 2. Illustration of Magnetic Mirror Confinement in Vicinity of Jupiter A second, related magnetic method is to join the ends of the solenoid together as a toroid, confining the plasma to a ring. A simple toroidal (i.e., circular) field, however, provides poor confinement because the radial gradient of the magnetic field strength results in plasma drift. A method to reduce drift and produce a stable plasma equilibrium is to superpose a poloidal magnetic field with the toroidal field, thus driving a current through the plasma itself. This provides a path for the plasma moving along the outer edge of the toroid to migrate to the inner edge and vice versa. This is the method used in tokamak systems (shown in Figure 3). Another solution has been to structurally modify the toroid chamber into a figure-eight configuration. This allowed plasma to spend half of the time on the inner portion of the tube, and half of the time on the outer portion of the tube. Such systems are called stellarators. This configuration has eventually evolved back into a (non-axially symmetric) toroidal configuration; rotating the windings in such a manner produces a stable plasma equilibrium while eliminating the need for a toroidal magnetic field. The fundamental issue with these confinement systems is that they require superconducting magnetic coils, pressure vessels, and neutron-energy-absorbing blankets for a 6-meter major radius by 6-meter high plasma, an enormous technological undertaking-and that is just for an ignition demonstration (see Chapter 5). Figure 3. a) Tokamak and b) Stellarator Confinement UNCLASSIFIED//FOR OFFI&iIAk YS& &PtkY 6