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Reference scenario for an advanced deuterium power plant system

Proceedings of the 19th IEEE/IPSS Symposium on Fusion Engineering. 19th SOFE (Cat. No.02CH37231)

The proposal is to make large deuterium (D-D) magnetic fusion power plants in which some (most) of the tritium produced by fusion is removed and stored. This tritium will ultimately decay to helium-3 that will be recycled to supplement the helium-3 produced by fusion. Thus the dominant fusion becomes that of deuterium and helium-3. The tritium would be removed using ion cyclotron waves in a similar manner to that proposed by Chang et al, and tested on TEXTOR, for removing alpha particles from a D-T plasma. Interestingly, with this scheme it only takes about 25 years before the rate of helium-3 production is sufficient to support a doubling of such plants every decade, with very low tritium content. The importance of this is that the production of 14.1 MeV neutrons is substantially reduced over a standard catalyzed D-D plant and even more so over a D-T plant. To be specific, if 90% of the tritium can be removed, the first power plant will average only 5.8% 14.1 MeV neutron power, when averaged over 30 years of operation. (5.8% of total plasma fusion power, any blanket neutron gain is extra). Later generations will get down to less than 4% of 14.1 MeV neutrons by using surplus helium-3 from earlier power plant operation. Ultimately, in steady state, the 14.1 MeV fraction will be 3% of total plasma fusion power. Large tokamak power plants are used to illustrate the approach, because it is possible to use "ITER rules" to develop a consistent system. In reality, at large scale-5000 to 6000 MW thermal-other systems may turn out to be superior.

John Sheffield 11.2.00. Reference Scenario for an Advanced Deuterium Power Plant System John Sheffield. Oak Ridge National Laboratory, and Joint Institute for Energy and Environment at the University of Tennessee. Abstract The proposal is to make large deuterium (D-D) magnetic fusion power plants in which some (most) of the tritium produced by fusion is removed and stored. This tritium will ultimately decay to helium-3 that will be recycled to supplement the helium-3 produced by fusion. Thus the dominant fusion becomes that of deuterium and helium-3. The tritium would be removed using ion cyclotron waves in a similar manner to that proposed by Chang et al, and tested on TEXTOR, for removing alpha particles from a D-T plasma. Interestingly, with this scheme it only takes about 25 years before the rate of helium-3 production is sufficient to support a doubling of such plants every decade, with very low tritium content. The importance of this is that the production of 14.1 MeV neutrons is substantially reduced over a standard catalyzed D-D plant and even more so over a D-T plant. To be specific, if 90% of the tritium can be removed, the first power plant will average only 5.8% 14.1 MeV neutron power, when averaged over 30 years of operation. (5.8% of total plasma fusion power, any blanket neutron gain is extra). Later generations will get down to less than 4% of 14.1 MeV neutrons by using surplus helium-3 from earlier power plant operation. Ultimately, in steady state, the 14.1 MeV fraction will be 3% of total plasma fusion power. Large tokamak power plants are used to illustrate the approach, because it is possible to use “ITER rules” to develop a consistent system. In reality, at large scale – 5000 to 6000 MW thermal – other systems may turn out to be superior. C.S.Chang, “Control of Energetic Ion Confinement by Ion Cyclotron Range of Frequency Waves”, Phys. Fluids B 3 (1), 259, 1991. C.S.Chang et al., “Theory of Energetic Ion Transport Induced by Waves of Ion Cyclotron Range of Frequencies in a Tokamak Plasma”, Phys. Fluids B 3 (12), 3429, 1991. R.Koch et al., “Interaction of ICRF Waves with Fast Particles on TEXTOR”, Plasma Phys. Control. Fusion 37, A291, 1995. 1