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Smarter waste strategies: Helping deliver on the promise of advanced nuclear
At COP28, held in Dubai in 2023, a clear consensus emerged: Nuclear energy must be a cornerstone of the global clean energy transition. With electricity demand projected to soar as we decarbonize not just power but also industry, transport, and heat, the case for new nuclear is compelling. More than 20 countries committed to tripling global nuclear capacity by 2050. In the United States alone, the Department of Energy forecasts that the country’s current nuclear capacity could more than triple, adding 200 GW of new nuclear to the existing 95 GW by mid-century.
Osamu Mitarai, Hiroki Hasuyama, Yoshihisa Wakuta
Fusion Science and Technology | Volume 21 | Number 4 | July 1992 | Pages 2265-2283
Technical Paper | Special Issue on D-He Fusion / D-3He/Fusion Reactor | doi.org/10.13182/FST92-A29720
Articles are hosted by Taylor and Francis Online.
Ignition characteristics in deuterium-tritium (D-T) and D-3He tokamak reactors with spin-polarized fuels are presented by using the ignition access condition based on the generalized saddle point in the representation of . Enhancement of the D-T fusion cross section due to parallel spin polarization with respect to the magnetic field can reduce the confinement enhancement factor required for reaching ignition by ∼20% if fusion particle loss is not induced by the anisotropic fusion particle distribution. Spin polarization is thus effective when a D-T reactor is marginal for ignition. In D-3He fusion, it is more advantageous to use spin-polarized fuel in the heating phase than in the case of D-T fusion. The ignition toroidal beta value can be reduced by spin polarization from 12 ± 0.8 to 5.3 ± 0.5% in D-3He = 2:1 plasma and from 17 ± 0.5 to 6.5 ± 0.2% in D-3He = 1:1 plasma. The auxiliary heating power to reach ignition, which is rather large for D-3He fusion, can be reduced by a factor of 2 to 3 compared with the unpolarized case. For example, in the D-3He Tokamak Reactor, 350 MW of auxiliary heating power for D:3He = 2:1 and Ti(0)/Te(0) = 1 without spin polarization can be reduced to 190 MW with complete polarization of the deuterium and 3He ions. The deuterium-deuterium fusion suppression effect, if it exists, does not alter the ignition condition much. Various problems related to the spin polarization scheme are also discussed.
