Artigo Acesso aberto Revisado por pares

Optimization of fusion power density in the two-energy-component tokamak reactor

1975; IOP Publishing; Volume: 15; Issue: 3 Linguagem: Inglês

10.1088/0029-5515/15/3/011

ISSN

1741-4326

Autores

D.L. Jassby,

Tópico(s)

Particle accelerators and beam dynamics

Resumo

Fusion power density Pf is a critical parameter for certain fusion reactor applications such as fissile breeding. This paper considers the optimal plasma conditions for maximizing Pf in a beam-driven D-T tokamak reactor. Given Te=Ti and fixed total plasma pressure, there is an optimal neτE for maximizing Pf, i.e. neτE = 4 × 1012 to 2 × 1013 cm−3 · s for Te = 3 – 15 keV and 200-keV D beams. The corresponding = (beam pressure/bulk-plasma pressure) is 0.96 to 0.70. Pfmax increases as Te is reduced and can be an order of magnitude larger than the maximum Pf of a thermal reactor of the same beta, at any temperature. A lower practical limit to Te may be set by requiring a minimum beam power multiplication Qb. For the purpose of fissile breeding, the minimum Qb ∼ 0.8, requiring Te⪆ 4 keV if Z = 1.

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