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A Fission-Fusion Hybrid Reactor in Steady-State L-Mode Tokamak Configuration with Natural Uranium Mark Reed FUNFI Varenna, Italy September 13 th, 2011
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PART I: The Issue PART II: Fission PART III: Fusion PART IV: Conclusions
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PART I: The Issue Why this might be a good idea
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Contention Fission-fusion hybrids could actually be more viable than stand-alone fusion reactors and obviate some challenges of fission.
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Constraints D-T tokamaks Fully non-inductive (steady-state) Low confinement mode (L-mode) operation Pebble bed blanket with helium coolant Natural or depleted uranium Lithium-lead eutectic layer for tritium breeding (one triton per fusion neutron)
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PART II: Fission The maximum natural uranium blanket power gain
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Basic Layout Li-Pb natural uranium with He coolant shield
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Neutronics Methodology Developed a subcritical Monte Carlo code (benchmarked with MCNP) Treated uranium and lithium layers as elongated toroidal shells (quartic solutions for neutron path lengths) ENDF cross-sections and other nuclear data
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Blanket Variables Uranium toroidal layer thickness Lithium toroidal layer thickness Relative positioning of toroidal layers Homogenized uranium density (different pebble designs) Lithium enrichment Major and minor tokamak radii
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Layer Thickness Optimization
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Subcritical Neutron Multiplication k = 0.27 k 0 = 1.19
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Total Power Composition
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Fusion-Born Neutron Fate
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Fission Results Blanket power gain of 7 Tritium breeding ratio of 1.05 Uranium layer thickness of 18 cm Lithium enrichment of 90% 6 Li Helium coolant velocity ≈ 10 m/s
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PART III: Fusion The minimum tokamak size for steady-state L-mode operation
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0-D Tokamak Model Volume-averaged parameters Simply relate R, a, B, q*, P fus, and Q fus Current limit and safety factor (q* > 2) Greenwald density limit Troyon no-wall pressure limit (β N < 3) L-mode operation (H-89 scaling) Fully non-inductive (f NI ≈ 1) Solenoid flux approximately twice plasma flux
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Fusion power surface density P F /A S and fixed B max uniquely define each operating point 2 < R/a < 4 1 2 3 4 5 6 0-D Tokamak Relations
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Stand-Alone Fusion Reactor Q = 40, R/a = 2.6, B max = 15 T, P F /A S = 5 MW/m 2.
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Fission-Fusion Hybrid Reactor Q = 6.3, R/a = 3.1, B max = 15 T, P F /A S = 3 MW/m 2.
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Fusion Results Major radius of 5.2 m Aspect ratio of 2.8 Maximum on-coil magnetic field of 15 T Fusion gain of 6.7 Total fusion power of 1.7 GW Safety factor of 3.0 H 89 = 1.48 (L-mode)
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PART IV: Conclusions What this all means
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Fission-Fusion Advantages Fully non-inductive L-mode operation at small scale (low capital cost relative to pure fusion devices) Subcritical operation (flexibility and safety) Control of fission blanket indirectly through control of the tokamak plasma – fission blanket gain increases with time due to plutonium breeding No uranium enrichment (non-proliferation) Enhanced transmutation of long-lived fission products through (n,2n) reactions
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Conclusion Instead of complicating the already difficult challenges of fission and fusion, fission-fusion hybrids could actually simplify many difficult aspects of fission and fusion. A profusion of pro-fusion sentiment?
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Acknowledgements Prof. Ron Parker (fusion) Prof. Ben Forget (fission) M. Reed, R. Parker, B. Forget. “A Fission-Fusion Hybrid Reactor in L- Mode Tokamak Configuration with Natural Uranium”. PSFC/RR-11-1 (2011). MIT Plasma Science and Fusion Center (PSFC) report:
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Extra Slides
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L-mode and H-mode H-mode has rough profiles that create edge- localized modes (ELMs), the bane of current fusion research. L-mode does not give rise to ELMs but has lower power density. Some current hybrid designs are based on ITER (H-mode).
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Hybrid Power The fission blanket augments the fusion power.
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At large size, increases in temperature lead to operation at the maximum D-T rate coefficient. T near maximum provides inherent stability (negative reactivity coefficient) Absolute maximum limits feasible parameter space 66 keV T= 10 keV 100keV Log (D-T rate coefficient)
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