US20080123795A1 - Controllable long term operation of a nuclear reactor - Google Patents

Controllable long term operation of a nuclear reactor Download PDF

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Publication number
US20080123795A1
US20080123795A1 US11/605,933 US60593306A US2008123795A1 US 20080123795 A1 US20080123795 A1 US 20080123795A1 US 60593306 A US60593306 A US 60593306A US 2008123795 A1 US2008123795 A1 US 2008123795A1
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United States
Prior art keywords
nuclear fission
canceled
reactor
neutron
fuel
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US11/605,933
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English (en)
Inventor
Roderick A. Hyde
Muriel Y. Ishikawa
Nathan P. Myhrvold
Lowell L. Wood
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TerraPower LLC
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Searete LLC
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Priority to US11/605,933 priority Critical patent/US20080123795A1/en
Application filed by Searete LLC filed Critical Searete LLC
Assigned to SEARETE LLC reassignment SEARETE LLC ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: ISHIKAWA, MURIEL Y., WOOD, LOWELL L. JR., HYDE, RODERICK A., MYHRVOLD, NATHAN P.
Priority to KR1020097013475A priority patent/KR20090085145A/ko
Priority to CA002670919A priority patent/CA2670919A1/en
Priority to JP2009539275A priority patent/JP2010511173A/ja
Priority to EP07873828A priority patent/EP2097906A4/en
Priority to CN200780049972.8A priority patent/CN101589439B/zh
Priority to PCT/US2007/024375 priority patent/WO2008105856A2/en
Priority to US12/069,908 priority patent/US9230695B2/en
Priority to US12/069,907 priority patent/US9275759B2/en
Publication of US20080123795A1 publication Critical patent/US20080123795A1/en
Priority to US12/157,714 priority patent/US20090080587A1/en
Priority to US12/157,720 priority patent/US20090080588A1/en
Priority to US12/316,446 priority patent/US9831004B2/en
Priority to JP2013079884A priority patent/JP6026944B2/ja
Priority to US14/251,894 priority patent/US9305669B2/en
Assigned to TERRAPOWER, LLC reassignment TERRAPOWER, LLC ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: SEARETE LLC
Priority to US15/791,923 priority patent/US10706979B2/en
Abandoned legal-status Critical Current

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    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21C—NUCLEAR REACTORS
    • G21C15/00—Cooling arrangements within the pressure vessel containing the core; Selection of specific coolants
    • G21C15/24—Promoting flow of the coolant
    • G21C15/243—Promoting flow of the coolant for liquids
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21C—NUCLEAR REACTORS
    • G21C1/00—Reactor types
    • G21C1/02—Fast fission reactors, i.e. reactors not using a moderator ; Metal cooled reactors; Fast breeders
    • G21C1/022—Fast fission reactors, i.e. reactors not using a moderator ; Metal cooled reactors; Fast breeders characterised by the design or properties of the core
    • G21C1/026—Reactors not needing refueling, i.e. reactors of the type breed-and-burn, e.g. travelling or deflagration wave reactors or seed-blanket reactors
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21C—NUCLEAR REACTORS
    • G21C7/00—Control of nuclear reaction
    • G21C7/06—Control of nuclear reaction by application of neutron-absorbing material, i.e. material with absorption cross-section very much in excess of reflection cross-section
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21C—NUCLEAR REACTORS
    • G21C15/00—Cooling arrangements within the pressure vessel containing the core; Selection of specific coolants
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21C—NUCLEAR REACTORS
    • G21C15/00—Cooling arrangements within the pressure vessel containing the core; Selection of specific coolants
    • G21C15/02—Arrangements or disposition of passages in which heat is transferred to the coolant; Coolant flow control devices
    • G21C15/04—Arrangements or disposition of passages in which heat is transferred to the coolant; Coolant flow control devices from fissile or breeder material
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21C—NUCLEAR REACTORS
    • G21C15/00—Cooling arrangements within the pressure vessel containing the core; Selection of specific coolants
    • G21C15/24—Promoting flow of the coolant
    • G21C15/243—Promoting flow of the coolant for liquids
    • G21C15/247—Promoting flow of the coolant for liquids for liquid metals
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21C—NUCLEAR REACTORS
    • G21C15/00—Cooling arrangements within the pressure vessel containing the core; Selection of specific coolants
    • G21C15/28—Selection of specific coolants ; Additions to the reactor coolants, e.g. against moderator corrosion
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21C—NUCLEAR REACTORS
    • G21C7/00—Control of nuclear reaction
    • G21C7/02—Control of nuclear reaction by using self-regulating properties of reactor materials, e.g. Doppler effect
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21D—NUCLEAR POWER PLANT
    • G21D3/00—Control of nuclear power plant
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E30/00—Energy generation of nuclear origin
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E30/00—Energy generation of nuclear origin
    • Y02E30/30—Nuclear fission reactors

Definitions

  • the present application relates to nuclear reactors, and systems, applications, and apparatuses related thereto.
  • Exemplary embodiments provide automated nuclear fission reactors and methods for their operation. Exemplary embodiments and aspects include, without limitation, re-use of nuclear fission fuel, alternate fuels and fuel geometries, modular fuel cores, fast fluid cooling, variable burn-up, programmable nuclear thermostats, fast flux irradiation, temperature-driven neutron absorption, low coolant temperature cores, refueling, and the like.
  • FIG. 1A schematically illustrates an exemplary nuclear fission reactor
  • FIGS. 1B and 1C plot cross-section versus neutron energy
  • FIGS. 1D through 1H illustrate relative concentrations during times at operation of a nuclear fission reactor at power
  • FIGS. 1I and 1J schematically illustrate an exemplary nuclear fission reactor core assembly
  • FIGS. 2A through 2C schematically illustrate exemplary nuclear fission fuel assemblies
  • FIGS. 3A through 3D schematically illustrate exemplary nuclear fission fuel geometries
  • FIG. 4 schematically illustrates exemplary non-contiguous nuclear fission fuel material
  • FIG. 5 schematically illustrates an exemplary modular nuclear fission fuel core
  • FIGS. 6A through 6C schematically illustrate an exemplary modular nuclear fission facility
  • FIG. 7 schematically illustrates exemplary fast fluid cooling
  • FIG. 8 schematically illustrates exemplary variable burn-up of nuclear fission fuel
  • FIG. 9A schematically illustrates exemplary programmable thermostating of nuclear fission fuel
  • FIG. 9B plots operating temperature profiles
  • FIGS. 10A and 10B schematically illustrate exemplary nuclear irradiation of material
  • FIGS. 11A through 11C schematically illustrate exemplary temperature control of nuclear reactivity
  • FIG. 12 schematically illustrates an exemplary low-coolant-temperature nuclear fission reactor
  • FIG. 13 schematically illustrates exemplary removal of nuclear fission fuel
  • FIGS. 14A and 14B schematically illustrate exemplary re-propagation of a nuclear fission deflagration wave.
  • embodiments provide automated nuclear fission reactors and methods for their operation. Details of an exemplary reactor, exemplary core nucleonics, and operations, all given by way of non-limiting example, will be set forth first. Then, details will be set forth regarding several exemplary embodiments and aspects, such as without limitation re-use of nuclear fission fuel, alternate fuels and fuel geometries, modular fuel cores, fast fluid cooling, variable burn-up, programmable nuclear thermostats, fast flux irradiation, temperature-driven neutron absorption, low coolant temperature cores, refueling, and the like.
  • a nuclear fission reactor 10 acts as an exemplary host environment for embodiments and aspects described herein. While many embodiments of the reactor 10 are contemplated, a common feature among many contemplated embodiments of the reactor 10 is origination and propagation of a nuclear fission deflagration wave, or “burnfront”.
  • Nuclear fission fuels envisioned for use in embodiments of the reactor 10 are typically widely available, such as without limitation uranium (natural, depleted, or enriched), thorium, plutonium, or even previously-burned nuclear fission fuel assemblies.
  • Other, less widely available nuclear fission fuels, such as without limitation other actinide elements or isotopes thereof may be used in embodiments of the reactor 10 .
  • embodiments of the reactor 10 contemplate long-term operation at full power on the order of around 1 ⁇ 3 century to around 1 ⁇ 2 century or longer, an aspect of some embodiments of the reactor 10 does not contemplate nuclear refueling (but instead contemplate burial in-place at ends-of-life) while some aspects of embodiments of the reactor 10 contemplate nuclear refueling—with some nuclear refueling occurring during shutdown and some nuclear refueling occurring during operation at power. It is also contemplated that nuclear fission fuel reprocessing may be avoided, thereby mitigating possibilities for diversion to military uses and other issues.
  • reactor 10 may be able to mitigate damage due to operator error, casualties such as a loss of coolant accident (LOCA), or the like. In some aspects decommissioning may be effected in low-risk and inexpensive manner.
  • LOCA loss of coolant accident
  • some embodiments of the reactor 10 may entail underground siting, thereby addressing large, abrupt releases and small, steady-state releases of radioactivity into the biosphere. Some embodiments of the reactor 10 may entail minimizing operator controls, thereby automating those embodiments as much as practicable. In some embodiments, a life-cycle-oriented design is contemplated, wherein those embodiments of the reactor 10 can operate from startup to shutdown at end-of-life in as fully-automatic manner as practicable. Some embodiments of the reactor 10 lend themselves to modularized construction. Finally, some embodiments of the reactor 10 may be designed according to high power density.
  • ⁇ T a negative temperature coefficient of reactivity
  • ⁇ T a distributed thermostat enables a propagating nuclear fission deflagration wave mode of nuclear fission fuel burn.
  • This mode simultaneously permits a high average burn-up of non-enriched actinide fuels, such as natural uranium or thorium, and use of a comparatively small “nuclear fission igniter” region of moderate isotopic enrichment of nuclear fissionable materials in the core's fuel charge.
  • non-enriched actinide fuels such as natural uranium or thorium
  • a comparatively small “nuclear fission igniter” region of moderate isotopic enrichment of nuclear fissionable materials in the core's fuel charge may be used as a comparatively small “nuclear fission igniter” region of moderate isotopic enrichment of nuclear fissionable materials in the core's fuel charge.
  • multiple redundancy is provided in primary and secondary core cooling.
  • an exemplary embodiment of the reactor 10 includes a nuclear fission reactor core assembly 100 that is disposed within a reactor pressure vessel 12 .
  • a nuclear fission reactor core assembly 100 that is disposed within a reactor pressure vessel 12 .
  • Some of the features that will be discussed later in detail regarding the nuclear fission reactor core assembly 100 include nuclear fission fuel materials and their respective nucleonics, fuel assemblies, fuel geometries, and initiation and propagation of nuclear fission deflagration waves.
  • the reactor pressure vessel 12 suitably is any acceptable pressure vessel known in the art and may be made from any materials acceptable for use in reactor pressure vessels, such as without limitation stainless steel.
  • a neutron reflector (not shown) and a radiation shield (not shown) surround the nuclear fission reactor core assembly 100 .
  • the reactor pressure vessel 12 is sited underground. In such cases, the reactor pressure vessel 12 can also function as a burial cask for the nuclear fission reactor core assembly 100 .
  • the reactor pressure vessel 12 suitably is surrounded by a region (not shown) of isolation material, such as dry sand, for long-term environmental isolation.
  • the region (not shown) of isolation material may have a size of around 100 m in diameter or so.
  • the reactor pressure vessel 12 is sited on or toward the Earth's surface.
  • Reactor coolant loops 14 transfer heat from nuclear fission in the nuclear fission reactor core assembly 100 to application heat exchangers 16 .
  • the reactor coolant may be selected as desired for a particular application.
  • the reactor coolant suitably is helium (He) gas.
  • the reactor coolant suitably may be other pressurized inert gases, such as neon, argon, krypton, xenon, or other fluids such as water or gaseous or superfluidic carbon dioxide, or liquid metals, such as sodium or lead, or metal alloys, such as Pb—Bi, or organic coolants, such as polyphenyls, or fluorocarbons.
  • the reactor coolant loops suitably may be made from tantalum (Ta), tungsten (W), aluminum (Al), steel or other ferrous or non-iron groups alloys or titanium or zirconium-based alloys, or from other metals and alloys, or from other structural materials or composites, as desired.
  • the application heat exchangers 16 may be steam generators that generate steam that is provided as a prime mover for rotating machinery, such as electrical turbine-generators 18 within an electrical generating station 20 .
  • the nuclear fission reactor core assembly 100 suitably operates at a high operating pressure and temperature, such as above 1,000K or so and the steam generated in the steam generator may be superheated steam.
  • the application heat exchanger 16 may be any steam generator that generates steam at lower pressures and temperatures (that is, need not be not superheated steam) and the nuclear fission reactor core assembly 100 operates at temperatures less than around 550K. In these cases, the application heat exchangers 16 may provide process heat for applications such as desalination plants for seawater or for processing biomass by distillation into ethanol, or the like.
  • Optional reactor coolant pumps 22 circulate reactor coolant through the nuclear fission reactor core assembly 100 and the application heat exchangers 16 .
  • the reactor coolant pumps 22 suitably are provided when the nuclear fission reactor core assembly 100 is sited approximately vertically coplanar with the application heat exchangers 16 , such that thermal driving head is not generated.
  • the reactor coolant pumps 22 may also be provided when the nuclear fission reactor core assembly 100 is sited underground.
  • thermal driving head may be developed between the reactor coolant exiting the reactor pressure vessel 12 and the reactor coolant exiting the application heat exchangers 16 at a lower temperature than the reactor coolant exiting the reactor pressure vessel 12 .
  • the reactor coolant pumps 22 need not be provided in order to provide sufficient circulation of reactor coolant through the nuclear fission reactor core assembly 100 to remove heat from fission during operation at power.
  • more than one reactor coolant loop 14 may be provided, thereby providing redundancy in the event of a casualty, such as a loss of coolant accident (LOCA) or a loss of flow accident (LOFA) or a primary-to-secondary leak or the like, to any one of the other reactor coolant loops 14 .
  • LOCA loss of coolant accident
  • LOFA loss of flow accident
  • Each reactor coolant loop 14 is typically rated for full-power operation, though some applications may remove this constraint.
  • one-time closures 24 are provided in lines of the reactor coolant system 14 .
  • a closure 24 is provided in an outlet line from the reactor pressure vessel 12 and in a return line to the reactor pressure vessel 12 from an outlet of the application heat exchanger 16 .
  • the one-time closures 24 are fast-acting closures that shut quickly under emergency conditions, such as detection of significant fission-product entrainment in reactor coolant).
  • the one-time closures 24 are provided in addition to a redundant system of automatically-actuated conventional valves (not shown).
  • Heat-dump heat exchangers 26 are provided for removal of after-life heat (decay heat).
  • the heat-dump heat exchanger 26 includes a primary loop that is configured to circulate decay heat removal coolant through the nuclear fission reactor core assembly 100 .
  • the heat-dump heat exchanger 26 includes a secondary loop that is coupled to an engineered heat-dump heat pipe network (not shown). In some situations, for example, for redundancy purposes, more than one the heat-dump heat exchanger 26 may be provided.
  • Each of the heat-dump heat exchangers 26 provided may be sited at a vertical distance above the nuclear fission reactor core assembly 100 so sufficient thermal driving head is provided to enable natural flow of decay heat removal coolant without need for decay heat removal coolant pumps. However, in some embodiments decay heat removal pumps (not shown) may be provided or, if provided, the reactor coolant pumps may be used for decay heat removal, where appropriate.
  • nuclear fission reactor core assembly 100 An overview of the nuclear fission reactor core assembly 100 and its nucleonics and propagation of a nuclear fission deflagration wave will be set forth first, followed by descriptions of exemplary embodiments and other aspects of the nuclear fission reactor core assembly 100 .
  • structural components of the reactor core assembly 100 may be made of tantalum (Ta), tungsten (W), rhenium (Re), or carbon composite, ceramics, or the like. These materials are suitable because of the high temperatures at which the nuclear fission reactor core assembly 100 operates, and because of their creep resistance over the envisioned lifetime of full power operation, mechanical workability, and corrosion resistance.
  • Structural components can be made from single materials, or from combinations of materials (e.g., coatings, alloys, multilayers, composites, and the like).
  • the reactor core assembly 100 operates at sufficiently lower temperatures so that other materials, such as aluminum (Al), steel, titanium (Ti) or the like can be used, alone or in combinations, for structural components.
  • the nuclear fission reactor core assembly 100 suitably is a breeder for reasons of efficient nuclear fission fuel utilization and of minimization of requirements for isotopic enrichment. Further, and referring now to FIGS. 1B and 1C , the nuclear fission reactor core assembly 100 suitably utilizes a fast neutron spectrum because the high absorption cross-section of fission products for thermal neutrons does not permit utilization of more than about 1% of thorium or of the more abundant uranium isotope, U 238 , in uranium-fueled embodiments, without removal of fission products.
  • FIG. 1B cross-sections for the dominant neutron-driven nuclear reactions of interest for the Th 232 -fueled embodiments are plotted over the neutron energy range 10 ⁇ 3 -10 7 eV. It can be seen that losses to radiative capture on fission product nuclei dominate neutron economies at near-thermal ( ⁇ 0.1 eV) energies, but are comparatively negligible above the resonance capture region (between 3-300 eV). Thus, operating with a fast neutron spectrum when attempting to realize a high-gain fertile-to-fissile breeder can help to preclude fuel recycling (that is, periodic or continuous removal of fission products).
  • the radiative capture cross-sections for fission products shown are those for intermediate-Z nuclei resulting from fast neutron-induced fission that have undergone subsequent beta-decay to negligible extents.
  • Those in the central portions of the burn-waves of embodiments of the nuclear fission reactor core assembly 100 will have undergone some decay and thus will have somewhat higher neutron avidity.
  • parameter studies have indicated that core fuel-burning results may be insensitive to the precise degree of such decay.
  • FIG. 1C cross-sections for the dominant neutron-driven nuclear reactions of primary interest for the Th 232 -fueled embodiments are plotted over the most interesting portion of the neutron energy range, between >10 4 and ⁇ 106.5 eV, in the upper portion of FIG. 1C .
  • the neutron spectrum of embodiments of the reactor 10 peaks in the ⁇ 10 5 eV neutron energy region.
  • the lower portion of FIG. 1C contains the ratio of these cross-sections vs.
  • the fertile-to-fissile breeding step (as the resulting Th 233 swiftly beta-decays to Pa 233 , which then relatively slowly beta-decays to U 233 , analogously to the U 239 —Np 239 —Pu 239 beta decay-chain upon neutron capture by U 238 ).
  • the nuclear fission deflagration wave within the nuclear fission reactor core assembly 100 will now be explained. Propagation of deflagration burning-waves through combustible materials can release power at a predictable level. Moreover, if the material configuration has the requisite time-invariant features, the ensuing power production may be at a steady level. Finally, if deflagration wave propagation-speed may be externally modulated in a practical manner, the energy release-rate and thus power production may be controlled as desired.
  • steady-state nuclear fission detonation waves are not generally appropriate for power production, such as for electrical power generation and the like.
  • nuclear fission deflagration waves are rare in nature, due to having to prevent the initial nuclear fission fuel configuration from disassembling as a hydrodynamic consequence of energy release during the earliest phases of wave propagation.
  • a nuclear fission deflagration wave can be initiated and propagated in a sub-sonic manner in fissionable fuel whose pressure is substantially independent of its temperature, so that its hydrodynamics is substantially ‘clamped’.
  • the nuclear fission deflagration wave's propagation speed within the nuclear fission reactor core assembly 100 can be controlled in a manner conducive to large-scale civilian power generation, such as in an electricity-producing reactor system like embodiments of the reactor 10 .
  • Nucleonics of the nuclear fission deflagration wave are explained below. Inducing nuclear fission of selected isotopes of the actinide elements—the fissile ones—by capture of neutrons of any energy permits the release of nuclear binding energy at any material temperature, including arbitrarily low ones. Release of more than a single neutron per neutron captured, on the average, by nuclear fission of substantially any actinide isotope admits the possibility-in-principle of a diverging neutron-mediated nuclear-fission chain reaction in such materials.
  • the characteristic speed of wave advance is of the order of the ratio of the distance traveled by a neutron from its fission-birth to its radiative capture on a fertile nucleus to the half-life of the (longest-lived nucleus in the chain of) beta-decay leading from the fertile nucleus to the fissile one.
  • the characteristic wave-speed is 10 ⁇ 4 -10 ⁇ 7 cm sec ⁇ 1 , or 10 ⁇ 13 -10 ⁇ 14 of that of a nuclear detonation wave.
  • Such a “glacial” speed-of-advance makes clear that the wave is that of a deflagration wave, not of a detonation wave.
  • the deflagration wave propagates not only very slowly but very stably. If such a wave attempts to accelerate, its leading-edge counters ever-more-pure fertile material (which is quite lossy in a neutronic sense), for the concentration of fissile nuclei well ahead of the center of the wave becomes exponentially low, and thus the wave's leading-edge (referred to herein as a “burnfront”) stalls. Conversely, if the wave slows, however, the local concentration of fissile nuclei arising from continuing beta-decay increases, the local rates of fission and neutron production rise, and the wave's leading-edge, that is the burnfront, accelerates.
  • the propagation may take place at an arbitrarily low material temperature—although the temperatures of both the neutrons and the fissioning nuclei may be around 1 MeV.
  • fissile isotopes of actinide elements are rare terrestrially, both absolutely and relative to fertile isotopes of these elements, fissile isotopes can be concentrated, enriched and synthesized.
  • the use of both naturally-occurring and man-made ones, such as U 235 and Pu 239 , respectively, in initiating and propagating nuclear fission detonation waves is well-known.
  • the algebraic sign of the function ⁇ ( ⁇ 2) constitutes a necessary condition for the feasibility of nuclear fission deflagration wave propagation in fertile material compared with the overall fissile isotopic mass budget, in the absence of neutron leakage from the core or parasitic absorptions (such as on fission products) within its body, for each of the fissile isotopes of the nuclear fission reactor core assembly 100 .
  • the algebraic sign is generally positive for all fissile isotopes of interest, from fission neutron-energies of approximately 1 MeV down into the resonance capture region.
  • the quantity ⁇ ( ⁇ 2)/ ⁇ upper-bounds the fraction of total fission-born neutrons which may be lost to leakage, parasitic absorption, or geometric divergence during deflagration wave propagation. It is noted that this fraction is 0.15-0.30 for the major fissile isotopes over the range of neutron energies which prevails in all effectively unmoderated actinide isotopic configurations of practical interest (approximately 0.1-1.5 MeV). In contrast to the situation prevailing for neutrons of (epi-) thermal energy (see FIG.
  • fissile element generation by capture on fertile isotopes is favored over fission-product capture by 0.7-1.5 orders-of-magnitude over the neutron energy range 0.1-1.5 MeV.
  • the former suggests that fertile-to-fissile conversion will be feasible only to the extent of 1.5-5% percent at-or-near thermal neutron energies, while the latter indicates that conversions in excess of 50% may be expected for near-fission energy neutron spectra.
  • fission neutrons in these actinide isotopes will likely result in either capture on a fertile isotopic nucleus or fission of a fissile one before neutron energy has decreased significantly below 0.1 MeV (and thereupon becomes susceptible with non-negligible likelihood to capture on a fission-product nucleus).
  • fission product nuclei concentrations must significantly exceed fertile ones and fissile nuclear concentrations may be an order-of-magnitude less than the lesser of fission-product or fertile ones before it becomes quantitatively questionable.
  • a basic condition on the ‘local’ geometry of the breeding-and-burning wave is that the flux history of neutrons excess to the local fissioning process in the core of the burn wave be quantitatively sufficient to at-least-reproduce the fissile atom density 1-2 mean-free-paths into the yet-unburned fuel, in a self-consistent sense.
  • the ‘ash’ behind the burn-wave's peak is substantially ‘neutronically neutral’ in such an accounting scheme, since the neutronic reactivity of its fissile fraction is just balanced by the parasitic absorptions of structure and fission product inventories on top of leakage.
  • the fissile atom inventory in the wave's center and just in advance of it is time-stationary as the wave propagates, then it's doing so stably; if less, then the wave is ‘dying’, while if more, the wave may be said to be ‘accelerating.’
  • a nuclear fission deflagration wave may be propagated and maintained in substantially steady-state conditions for long time intervals in configurations of naturally-occurring actinide isotopes.
  • Propagation of a nuclear fission deflagration wave has implications for embodiments of the nuclear fission reactor 10 .
  • local material temperature feedback can be imposed on the local nuclear reaction rate at an acceptable expense in the deflagration wave's neutron economy.
  • Such a large negative temperature coefficient of neutronic reactivity confers an ability to control the speed-of-advance of the deflagration wave. If very little thermal power is extracted from the burning fuel, its temperature rises and the temperature-dependent reactivity falls, and the nuclear fission rate at wave-center becomes correspondingly small and the wave's equation-of-time reflects only a very small axial rate-of-advance.
  • the local material-temperature thermostating modules may use around 5-10% of the total fission neutron production in the nuclear fission reactor 10 .
  • Another ⁇ 10% of the total fission neutron production in the nuclear fission reactor 10 may be lost to parasitic absorption in the relatively large quantities of high-performance, high temperature, structure materials (such as Ta, W, or Re) employed in structural components of the nuclear fission reactor 10 .
  • the Zs of these materials are approximately 80% of that of the actinides, and thus their radiative capture cross-sections for high-energy neutrons are not particularly small compared to those of the actinides, as is indicated for Ta in FIGS. 1B and 1C .
  • a final 5-10% of the total fission neutron production in the nuclear fission reactor 10 may be lost to parasitic absorption in fission products.
  • the neutron economy characteristically is sufficiently rich that approximately 0.7 of total fission neutron production is sufficient to sustain deflagration wave-propagation in the absence of leakage and rapid geometric divergence. This is in sharp contrast with (epi) thermal-neutron power reactors employing low-enrichment fuel, for which neutron-economy discipline in design and operation must be strict.
  • features of the fuel-charge of embodiments of the nuclear fission reactor core assembly 100 are depicted at four equi-spaced times during the operational life of the reactor after origination of the nuclear fission deflagration wave (sometimes referred to herein as “nuclear fission ignition”) in a scenario in which full reactor power is continuously demanded over a 1 ⁇ 3 century time-interval.
  • nuclear fission deflagration wave sometimes referred to herein as “nuclear fission ignition”
  • two nuclear fission deflagration wavefronts propagate from an origination point 28 (near the center of the nuclear fission reactor core assembly 100 ) toward ends of the nuclear fission reactor core assembly 100 .
  • FIGS. 1E , 1 F, 1 G, and 1 G illustrate masses (in kg of total mass per cm of axial core-length) of various isotopic components in a set of representative near-axial zones and fuel specific power (in W/g) at the indicated axial position as ordinate-values versus axial position along an exemplary, non-limiting 10-meter-length of the fuel-charge as an abscissal value at approximate times after nuclear fission ignition of approximately 7.5 years, 15 years, 22.5 years, and 30 years, respectively.
  • the central perturbation is due to the presence of the nuclear fission igniter module indicated by the origination point 28 ( FIG. 1D ).
  • the neutron flux from the most intensely burning region behind the burnfront breeds a fissile isotope-rich region at the burnfront's leading-edge, thereby serving to advance the nuclear fission deflagration wave.
  • the nuclear fission deflagration wave's burnfront has swept over a given mass of fuel, the fissile atom concentration continues to rise for as long as radiative capture of neutrons on available fertile nuclei is considerably more likely than on fission product nuclei, while ongoing fission generates an ever-greater mass of fission products.
  • Nuclear power-production density peaks in this region of the fuel-charge, at any given moment.
  • differing actions of two slightly different types of thermostating units on the left and the right sides of the igniter module account for the corresponding slightly differing power production levels.
  • FIGS. 1D-1H it can be seen that well behind the nuclear fission deflagration wave's advancing burnfront, the concentration ratio of fission product nuclei (whose mass closely averages half that of a fissile nucleus) to fissile ones climbs to a value comparable to the ratio of the fissile fission to the fission product radiative capture cross-sections ( FIG. 1B ), the “local neutronic reactivity” thereupon goes slightly negative, and both burning and breeding effectively cease—as will be appreciated from comparing FIGS. 1E , 1 F, 1 G, and 1 H with each other, far behind the nuclear fission deflagration wave burnfront.
  • all the nuclear fission fuel ever used in the reactor is installed during manufacture of the nuclear fission reactor core assembly 100 , and no spent fuel is ever removed from the nuclear fission reactor core assembly 100 , which is never accessed after nuclear fission ignition.
  • additional nuclear fission fuel is added to the nuclear fission reactor core assembly 100 after nuclear fission ignition.
  • spent fuel is removed from the reactor core assembly (and, in some embodiments, removal of spent fuel from the nuclear fission reactor core assembly 100 may be performed while the nuclear fission reactor 10 is operating at power).
  • pre-expansion of the as-loaded fuel permits higher-density actinides to be replaced with lower-density fission products without any overall volume changes in fuel elements, as the nuclear fission deflagration wave sweeps over any given axial element of actinide ‘fuel,’ converting it into fission-product ‘ash.’
  • nuclear fission igniter modules enriched in fissile isotopes. Higher enrichments result in more compact modules, and minimum mass modules may employ moderator concentration gradients.
  • nuclear fission igniter module design may be determined in part by non-technical considerations, such as resistance to materials diversion for military purposes in various scenarios.
  • Such modules may employ U 235 in U 238 , in sufficiently low concentration as to be effectively non-detonatable in any quantity or configuration—such as ⁇ 20%—in contrast, for example, to technically more optimal Pu 239 in Th 232 .
  • nuclear fission igniters included nuclear fission material configured to initiate propagation of the burning wavefront
  • the nuclear fission igniter may include other types of reactivity sources in addition to or in place of those previously described.
  • nuclear fission igniters may include “burning embers”, e.g., nuclear fission fuel enriched in fissile isotopes via exposure to neutrons within a propagating nuclear fission deflagration wave reactor. Such “burning embers” may function as nuclear fission igniters, despite the presence of various amounts of fission products “ash”.
  • nuclear fission igniters may include neutron sources using electrically driven sources of high energy ions (such as protons, deuterons, alpha particles, or the like) or electrons that may in turn produce neutrons.
  • a particle accelerator such as a linear accelerator may be positioned to provide high energy protons to an intermediate material that may in turn provide such neutrons (e.g., through spallation).
  • a particle accelerator such as a linear accelerator may be positioned to provide high energy electrons to an intermediate material that may in turn provide such neutrons (e.g., by electro-fission and/or photofission of high-Z elements).
  • other known neutron emissive processes and structures such as electrically induced fusion approaches, may provide neutrons (e.g., 14 Mev neutrons from D-T fusion) that may thereby initiate the propagating fission wave.
  • a centrally-positioned nuclear fission igniter moderately enriched in fissionable material, such as U 235 has a neutron-absorbing material (such as a borohydride) removed from it (such as by operator-commanded electrical heating), and the nuclear fission igniter becomes neutronically critical.
  • a neutron-absorbing material such as a borohydride
  • Local fuel temperature rises to a design set-point and is regulated thereafter by the local thermostating modules (discussed in detail later).
  • Neutrons from the fast fission of U 235 are mostly captured at first on local U 238 or Th 232 .
  • uranium enrichment of the nuclear fission igniter may be reduced to levels not much greater than that of light water reactor (LWR) fuel by introduction into the nuclear fission igniter and the fuel region immediately surrounding it of a radial density gradient of a refractory moderator, such as graphite.
  • LWR light water reactor
  • High moderator density enables low-enrichment fuel to burn satisfactorily, while decreasing moderator density permits efficient fissile breeding to occur.
  • optimum nuclear fission igniter design may involve trade-offs between proliferation robustness and the minimum latency from initial criticality to the availability of full-rated-power from the fully-ignited fuel-charge of the core.
  • Lower nuclear fission igniter enrichments entail more breeding generations and thus impose longer latencies.
  • the maximum (unregulated) reactivity of the nuclear fission reactor core assembly 100 slowly decreases in the first phase of the nuclear fission ignition process because, although the total fissile isotope inventory is increasing monotonically, this total inventory is becoming more spatially dispersed.
  • the maximum reactivity may be arranged for the maximum reactivity to still be slightly positive at the time-point at which its minimum value is attained.
  • the maximum reactivity begins to increase rapidly toward its greatest value, corresponding to the fissile isotope inventory in the region of breeding substantially exceeding that remaining in the nuclear fission igniter.
  • a quasi-spherical annular shell then provides maximum specific power production.
  • the fuel-charge of the nuclear fission reactor core assembly 100 is referred to as “ignited.”
  • nuclear fission reactor core assembly 100 has been “ignited”, propagation of the nuclear fission deflagration wave, also referred to herein as “nuclear fission burning”, will now be discussed.
  • the spherically-diverging shell of maximum specific nuclear power production continues to advance radially from the nuclear fission igniter toward the outer surface of the fuel charge. When it reaches this surface, it naturally breaks into two spherical zonal surfaces, with one surface propagating in each of the two opposite directions along the axis of the cylinder. At this time-point, the full thermal power production potential of the core has been developed.
  • This epoch is characterized as that of the launching of the two axially-propagating nuclear fission deflagration wave burnfronts.
  • the center of the core's fuel-charge is ignited, thus generating two oppositely-propagating waves.
  • This arrangement doubles the mass and volume of the core in which power production occurs at any given time, and thus decreases by two-fold the core's peak specific power generation, thereby quantitatively minimizing thermal transport challenges.
  • the core's fuel charge is ignited at one end, as desired for a particular application. In other embodiments, the core's fuel charge may be ignited in multiple sites.
  • the core's fuel charge is ignited at any 3-D location within the core as desired for a particular application.
  • two propagating nuclear fission deflagration waves will be initiated and propagate away from a nuclear fission ignition site, however, depending upon geometry, nuclear fission fuel composition, the action of neutron modifying control structures or other considerations, different numbers (e.g., one, three, or more) of nuclear fission deflagration waves may be initiated and propagated.
  • the discussion herein refers, without limitation, to propagation of two nuclear fission deflagration wave burnfronts.
  • the temperature of the two ends of the core decreases slightly below the thermostating modules' design set-point, a neutron absorber is thereby withdrawn from the corresponding sub-population of the core's thermostating modules, and the local neutron flux is permitted thereby to increase to bring the local thermal power production to the level which drives the local material temperature up to the set-point of the local thermostating modules.
  • this process is not effective in heating the coolant significantly until its two divided flows move into the two nuclear burn-fronts.
  • These two portions of the core's fuel-charge which are capable of producing significant levels of nuclear power when not suppressed by the neutron absorbers of the thermostating modules—then act to heat the coolant to the temperature specified by the design set-point of their modules, provided that the nuclear fission fuel temperature does not become excessive (and regardless of the temperature at which the coolant arrived in the core).
  • the two coolant flows then move through the two sections of already-burned fuel centerward of the two burnfronts, removing residual nuclear fission and afterheat thermal power from them, both exiting the fuel-charge at its center.
  • This arrangement encourages the propagation of the two burnfronts toward the two ends of the fuel-charge by “trimming” excess neutrons primarily from the trailing edge of each front, as illustrated in FIGS. 1E-1H .
  • Final, irreversible negation of the core's neutronic reactivity may be performed at any time by injection of neutronic poison into the coolant stream, via either the primary loops which extend to the application heat exchangers 16 ( FIG. 1A ) or the afterheat-dumping loops connecting the nuclear fission reactor 10 ( FIG. 1A ) to the heat dump heat exchangers 26 ( FIG. 1A ).
  • lightly loading the coolant stream with a material such as BF 3 may deposit metallic boron substantially uniformly over the inner walls of the coolant-tubes threading through the reactor's core, via exponential acceleration of the otherwise slow chemical reaction 2BF 3 +3H 2 ->2B+6HF by the high temperatures found therein.
  • a material such as BF 3
  • a volatile reducing agent such as H 2
  • Boron is a highly refractory metalloid, and will not migrate from its site of deposition.
  • Substantially uniform presence of boron in the core in ⁇ 100 kg quantities may negate the core's neutronic reactivity for indefinitely prolonged intervals without involving the use of powered mechanisms in the vicinity of the reactor.
  • the nuclear fission reactor core assembly 100 is suitable for use with a fast neutron spectrum nuclear fission reactor. It will be appreciated that the nuclear fission reactor core assembly 100 is shown schematically in FIG. 1I . As such, no geometric limitations are intended regarding shape of the nuclear fission reactor core assembly 100 . As mentioned above, details were discussed for circular cylinders of natural uranium or thorium metal that may stably propagate nuclear fission deflagration waves for arbitrarily great axial distances.
  • nuclear fission deflagration waves is not to be construed to be limited to circular cylinders or to metallic nuclear fission fuels, or to pure uranium or thorium nuclear fission fuel materials.
  • additional embodiments of alternate geometries of the nuclear fission reactor core assembly 100 and fuel charges disposed therein will be described later.
  • a neutron reflector/radiation shield 120 surrounds nuclear fission fuel 130 .
  • the nuclear fission fuel 130 is fissionable material, that is material appropriate for undergoing fission in a nuclear fission reactor, examples of which are actinide or transuranic elements.
  • the fissionable material for the nuclear fission fuel 130 may include without limitation Th 232 or U 238 . However, in other embodiments discussed below, other fissionable material may be used in the nuclear fission fuel 130 .
  • the nuclear fission fuel 130 is contiguous. In other embodiments, the nuclear fission fuel 130 is non-contiguous.
  • a nuclear fission igniter 110 acts within the nuclear fission fuel 130 for initiating a nuclear fission deflagration wave burnfront (not shown).
  • the nuclear fission igniter 110 is made and operates according to principles and details discussed above. Therefore, details of construction and operation of the nuclear fission igniter 110 need not be repeated for sake of brevity.
  • a propagating burnfront 140 that is, a propagating nuclear fission deflagration wave burnfront, as discussed above
  • a propagating burnfront 140 is initiated and propagates throughout the nuclear fission fuel 130 ( FIG. 1I ) a direction shown by an arrow 144 .
  • a region 150 of maximum reactivity is established around the propagating burnfront 140 .
  • the propagating burnfront 140 propagates through unburnt nuclear fission fuel 154 in the direction indicated by the arrow 144 , leaving behind the propagating burnfront 140 burnt nuclear fission fuel 160 that includes fission products 164 , such as isotopes of iodine, cesium, strontium, xenon, and/or barium (and referred to in the discussion above as “fission product ash”).
  • burnt nuclear fission fuel and unburnt nuclear fission fuel the term “burning” (as applied to nuclear fission fuel) means that at least some components of the nuclear fission fuel undergo neutron-mediated nuclear fission.
  • burning In the context of propagating nuclear fission deflagration wave burnfronts, the terms “burning” and “burnt” also mean that at least some components of the nuclear fission fuel undergo “breeding”, whereby neutron absorption is followed by multi-second half-life beta-decay transmutation into one or more fissile isotopes, which then may or may not undergo neutron-mediated nuclear fission.
  • the unburnt nuclear fission fuel 154 may be considered a first neutron environment having a first set of neutron environment parameters.
  • the burnt nuclear fission fuel 160 may be considered a second neutron environment having a second set of neutron environment parameters that are different than the first set of neutron environment parameters.
  • the term “neutron environment” refers to the detailed neutron distribution, including its variation with respect to time, space, direction, and energy.
  • the neutron environment includes the aggregate of multiple individual neutrons, each of which may occupy different locations at different times, and each of which may have different directions of motion and different energies. In some circumstances, a nuclear environment may be characterized by a reduced subset of these detailed properties.
  • a reduced subset may include an aggregation of all neutrons within given space, time, direction, and energy ranges of specified time, space, direction, and energy values.
  • some or all of the time, space, direction, or energy aggregations may incorporate value-dependent weighting functions.
  • a reduced subset may include weighted aggregation over the full range of direction and energy values.
  • the aggregation over energies may involve energy-dependent weighting by a specified energy function. Examples of such weighting functions include material and energy-dependent cross-sections, such as those for neutron absorption or fission.
  • the nuclear fission igniter 110 may be located as desired.
  • the nuclear fission igniter 110 may be located toward the center of the nuclear fission fuel 130 ( FIG. 1I ). In other embodiments (not shown) the nuclear fission igniter 110 may be located toward an end of the nuclear fission fuel 130 .
  • a propagating burnfront 141 is originated and propagated through the other fuel 154 along a direction indicated by an arrow 145 .
  • a region 151 of maximum reactivity is established around the obligating burnfront 141 .
  • the propagating burnfront 141 leaves behind it the burnt nuclear fission fuel 160 and the fission products 164 .
  • Principles and details of origination and propagation of the propagating burnfront 141 are the same as that previously discussed for the propagating burnfront 140 . Therefore, details of origination and propagation of the propagating burnfront 141 need not be provided for sake of brevity.
  • a nuclear fission reactor 200 such as a fast neutron spectrum nuclear fission reactor, includes nuclear fission fuel assemblies 210 disposed therein.
  • the following discussion includes details of exemplary nuclear fission fuel assemblies 210 that may be used in the nuclear fission reactor 200 .
  • Other details regarding the nuclear fission reactor 200 including origination and propagation of a nuclear fission deflagration wave burnfront (that is, “burning” the nuclear fission fuel) are similar to those of the nuclear fission reactor 10 ( FIG. 1A ), and need not be repeated for sake of brevity.
  • the nuclear fission fuel assembly 210 suitably includes a previously burnt nuclear fission fuel assembly 220 .
  • the previously burnt nuclear fission fuel assembly 220 is clad with cladding 224 .
  • the cladding 224 is the “original” cladding in which the previously burned nuclear fission fuel assembly 220 was clad.
  • the term “previously burnt” means that at least some components of the nuclear fission fuel assembly have undergone neutron-mediated nuclear fission and that the isotopic composition of the nuclear fission fuel has been modified.
  • a burnt nuclear fission fuel assembly 220 may have been previously burnt in any reactor, such as without limitation a light water reactor. It is intended that the previously burnt nuclear fission fuel assembly 220 can include without limitation any type of nuclear fissionable material whatsoever appropriate for undergoing fission in a nuclear fission reactor, such as actinide or transuranic elements like natural thorium, natural uranium, enriched uranium, or the like.
  • the previously burnt nuclear fission fuel assembly 220 may not be clad with “original” cladding 224 , but in these embodiments, the previously burnt nuclear fission fuel assembly 220 is chemically untreated subsequent to its previous burning in the nuclear fission reactor 200 .
  • the previously burnt nuclear fission fuel assembly 220 and its “original” cladding 224 is clad with cladding 230 .
  • the previously burnt nuclear fission fuel assembly 220 is retained in its original cladding 224 , and the cladding 230 is disposed around an exterior of the cladding 224 .
  • the cladding 230 can accommodate swelling.
  • the cladding 224 was sufficient to contain swelling at approximately 3% burn-up of the previously burnt nuclear fission fuel assembly 220 .
  • the cladding 230 contacts the cladding 224 at azimuthally, symmetric, cylindrical faces around the cladding 224 .
  • Such an arrangement enables removal of heat through the contacting faces while allowing at least one half of the cladding 224 to expand into void spaces between the cladding 224 and the cladding 230 .
  • the cladding 230 is made up of cladding sections (not shown) that are configured to help accommodate swelling into the void spaces, as described above.
  • the cladding 230 may be provided as a barrier, such as a tube, provided between an exterior of the cladding 224 and reactor coolant (not shown).
  • the previously burned nuclear fission fuel assembly 220 is burnt in the nuclear fission reactor 200 as the nuclear fission fuel assembly 210 . That is, the previously burnt nuclear fission fuel assembly 220 may not be clad with the cladding 230 .
  • This embodiment envisions burning the previously burnt nuclear fission fuel assembly 220 , such as one that was burnt in a light water reactor, or in a fast neutron spectrum nuclear fission reactor, or in any other form of nuclear fission reactor and either (a) tolerating or planning to accept possible failure of the cladding 224 due to swell or, (b) burning the previously burnt nuclear fission fuel assembly 220 in the fast neutron spectrum nuclear fission reactor 200 to levels significantly less than isotopic depletion (in which case swelling may be of acceptable magnitude).
  • Each of the nuclear fission fuel structures 310 , 320 , 330 , and 340 includes a nuclear fission igniter 300 , and a propagating nuclear fission deflagration wave 302 is propagated in a direction indicated by an arrow 304 .
  • the nuclear fission igniter 300 is disposed toward a center of the spherical nuclear fission fuel structure 310 .
  • the propagating burnfront 302 propagates radially outward from the nuclear fission igniter 300 , as indicated by the arrows 304 .
  • the nuclear fission igniter 300 is disposed as desired. As discussed above, two propagating burnfronts 302 may be originated and propagated toward ends of the parallelepiped nuclear fission fuel structure 320 along directions indicated by the arrows 304 . Alternately, the nuclear fission igniter 300 may be disposed toward an end of the parallelepiped nuclear fission fuel structure 320 , in which case one propagating burnfront 302 is originated and propagates toward the other end of the parallelepiped nuclear fission fuel structure 320 along the direction indicated by the arrow 304 .
  • the nuclear fission igniter 300 is disposed as desired.
  • Two propagating burnfronts 302 may be originated and propagated away from the nuclear fission igniter 300 and toward each other along directions indicated by the arrows 304 .
  • the toroidal nuclear fission fuel structure 330 may be considered to be “burnt” when the propagating burnfronts 302 meet, and propagation of the propagating burnfront 302 may stop.
  • only one propagating burnfront 302 is originated and propagates around the toroidal nuclear fission fuel structure 330 along the direction indicated by the arrow 304 .
  • the toroidal nuclear fission fuel structure 330 may be considered to be “burnt” when the propagating burnfront 302 returns to the site of the nuclear fission igniter 300 , and propagation of the propagating burnfront 302 may stop or may be re-started.
  • the propagating burnfront 302 is “restarted” due to the removal or decay of fission products during the burnfront's propagation around the toroid. In another embodiment, the propagating burnfront 302 is “restarted” due to control of neutron modifying structures, as discussed later.
  • the toroidal nuclear fission fuel structure 330 is not a “geometric” toroid, but a “logical” toroid, with a more general reentrant structure.
  • nuclear fission deflagration propagating wave burnfronts can be initiated and propagated in nuclear fission fuels having any shape as desired.
  • the nuclear fission igniter 300 can be located as desired.
  • Propagating burnfronts 302 are initiated and propagate along directions indicated by the arrows 304 as desired for a particular application.
  • thermal management may be adjusted to provide thermal control appropriate for any changes in operational parameters, such as revised neutronic action of the previously burnt or modified nuclear fission fuel or other parameter changes, that may result from removal of ash, addition of fuels, or from other parameters of re-burning.
  • the nuclear fission ignitor 300 may be any of the varieties of nuclear fission ignitor previously discussed.
  • the indicated nuclear fission ignitor 300 is the site at which nuclear fission ignition occurs, but for some embodiments (e.g., electrical neutron sources) additional components of the nuclear fission ignitor may exist, and may reside in different physical locations.
  • a nuclear fission fuel structure 400 includes a nuclear fission igniter 410 and non-contiguous segments 420 of nuclear fission fuel material.
  • the behavior of a nuclear fission deflagration wave with non-contiguous segments 420 of nuclear fission fuel material is similar to that previously discussed for contiguous nuclear fission fuel material; it is crucial only that the non-continguous segments 420 be in “neutronic” contact, not physical contact.
  • a modular nuclear fission fuel core 500 includes a neutron reflector/radiation shield 510 and modular nuclear fission fuel assemblies 520 .
  • the modular nuclear fission fuel assemblies 520 are placed as desired within the fuel assembly receptacles 530 .
  • the modular nuclear fission fuel core 500 may be operated in any number of ways. For example, all of the fuel assembly receptacles 530 in the modular nuclear fission fuel core 500 may be fully populated with modular nuclear fission fuel assemblies 520 prior to initial operation (e.g., prior to initial origination and propagation of a nuclear fission deflagration propagating wave burnfront within and through the modular nuclear fission fuel assemblies 520 ).
  • a nuclear fission deflagration wave burnfront may be removed from their respective fuel assembly receptacles 530 and replaced with unused modular nuclear fission fuel assemblies 540 , as desired; this emplacement is indicated by the arrow 544 .
  • a nuclear fission deflagration wave burnfront can be initiated in the unused modular nuclear fission fuel assemblies 540 , thereby enabling continued or extended operation of the modular nuclear fission fuel core 500 as desired.
  • the modular nuclear fission fuel core 500 need not be fully populated with modular nuclear fission fuel assemblies 520 prior to initial operation.
  • less than all of the fuel assembly receptacles 530 can be populated with modular nuclear fission fuel assemblies 520 .
  • the number of modular nuclear fission fuel assemblies 520 that are placed within the modular nuclear fission fuel core 500 can be determined based upon power demand, such as electrical loading in watts, that will be placed upon the modular nuclear fission fuel core 500 .
  • a nuclear fission deflagration wave burnfront is originated and propagated through the modular nuclear fission fuel assemblies 520 as previously described.
  • thermal management may be adjusted to provide thermal control appropriate to maintain the inserted fuel assembly receptacles 530 at appropriate temperatures.
  • the modular nuclear fission fuel core 500 again need not be fully populated with modular nuclear fission fuel assemblies 520 prior to initial operation.
  • the number of modular nuclear fission fuel assemblies 520 provided may be determined based upon a number of modular nuclear fission fuel assemblies 520 that are available or for other reasons.
  • a nuclear fission deflagration wave burnfront is originated and propagates through the modular nuclear fission fuel assemblies 520 .
  • the unpopulated fuel assembly receptacles 530 can be populated with modular nuclear fission fuel assemblies 520 , such as on a “just-in-time” basis; this emplacement is indicated by the arrow 544 .
  • continued or extended operation of the modular nuclear fission fuel core 500 can be enabled without initially fueling the entire modular nuclear fission fuel core 500 with modular nuclear fission fuel assemblies 520 .
  • a modular nuclear fission reactor can be populated with any number of nuclear fission reactor cores in the same manner that the modular nuclear fission fuel core 500 can be populated with any number of modular nuclear fission fuel assemblies 520 .
  • the modular nuclear fission reactor can be analogized to the modular nuclear fission fuel core 500 and nuclear fission reactor cores can be analogized to the modular nuclear fission fuel assemblies 520 .
  • the several contemplated modes of operation discussed above for the modular nuclear fission fuel core 500 thus apply by analogy to a modular nuclear fission reactor.
  • a nuclear fission facility 600 includes a fast neutron spectrum nuclear fission core assembly 610 that is operationally coupled to an operational sub system 620 (such as without limitation an electrical power generating facility) via a core-subsystem coupling 630 (such as without limitation a reactor coolant system such as a primary loop and, if desired, a secondary loop including a steam generator).
  • an operational sub system 620 such as without limitation an electrical power generating facility
  • a core-subsystem coupling 630 such as without limitation a reactor coolant system such as a primary loop and, if desired, a secondary loop including a steam generator.
  • another fast neutron spectrum nuclear fission core assembly 610 may be emplaced within the nuclear fission facility 600 .
  • the additional fast neutron spectrum nuclear fission core assembly 610 is operationally coupled to another operational sub system 620 by another core-subsystem coupling 630 .
  • the operational sub system's 620 are coupled to each other via a subsystem-subsystem coupling 640 .
  • a subsystem-subsystem coupling 640 can provide prime mover or other energy transfer medium between the operational sub systems 620 . To that end, energy produced by any one of the nuclear core assemblies 610 can be transferred to any operational sub system 620 as desired.
  • a third fast neutron spectrum nuclear fission core assembly 610 and associated operational sub system 620 , and core-subsystem coupling 630 have been placed in the nuclear fission facility 600 .
  • energy produced by any one of the fast neutron spectrum nuclear fission core assemblies 610 can be transferred to any operational sub system 620 as desired.
  • this linking process can be more general than discussed above, so that, the nuclear fission facility 600 may consist of a number N of fast neutron spectrum nuclear fission core assemblies 610 , and a same or different number M of operational subsystems 620 .
  • the individual nuclear fast neutron spectrum nuclear fission core assemblies 610 need not be identical to each other, nor need the operational sub systems 620 be identical to each other.
  • the core-subsystem couplings 630 need not be identical to each other, nor do the subsystem-subsystem couplings 640 need be identical to each other.
  • other embodiments of operational sub system 620 include, without limitation, reactor coolant systems, electrical nuclear fission ignitors, afterlife heat-dumps, reactor site facilities (such as basing and security), and the like.
  • heat energy can be extracted from a nuclear fission reactor core according to another embodiment.
  • a nuclear fission deflagration wave burnfront is initiated and propagated in a burning wavefront heat generating region 720 , in a manner as described above.
  • Heat absorbing material 710 such as a condensed phase density fluid (e.g., water, liquid metals, terphenyls, polyphenyls, fluorocarbons, FLIBE (2LiF—BeF2) and the like) flows through the region 720 as indicated by an arrow 750 , and heat is transferred from the propagating burnfront fission to the heat absorbing material 710 .
  • a condensed phase density fluid e.g., water, liquid metals, terphenyls, polyphenyls, fluorocarbons, FLIBE (2LiF—BeF2) and the like
  • the heat absorbing material 710 is chosen to be a nuclear inert material (such as He4) so as to minimally perturb the neutron spectrum.
  • the neutron content is sufficiently robust, so that a non-nuclear-inert heat absorbing material 710 may be acceptably utilized.
  • the heat absorbing material 710 flows to a heat extraction region 730 that is substantially out of thermal contact with the burning wavefront heat generating region 720 .
  • the energy 740 is extracted from the heat absorbing material 710 at the heat extraction region 730 .
  • the heat absorbing material 710 can reside in either a liquid state, a multiphase state, or a substantially gaseous state upon extraction of the heat energy 740 in the heat extraction region 730 .
  • a nuclear fission deflagration wave burnfront can be driven into areas of nuclear fission fuel as desired, thereby enabling a variable nuclear fission fuel burn-up.
  • a nuclear fission deflagration wave burnfront 810 is initiated and propagated as described above.
  • Actively controllable neutron modifying structures 830 can direct or move the burnfront 810 in directions indicated by areas 820 .
  • the actively controllable neutron modifying structures 830 insert neutron absorbers, such as without limitation Li6, B10, or Gd, into nuclear fission fuel behind the burnfront 810 , thereby driving down or lowering neutronic reactivity of fuel that is presently being burned by the burnfront 810 relative to neutronic reactivity of fuel ahead of the burnfront 810 , thereby speeding up the propagation rate of the nuclear fission deflagration wave.
  • the actively controllable neutron modifying structures 830 insert neutron absorbers into nuclear fission fuel ahead of the burnfront 810 , thereby slowing down the propagation of the nuclear fission deflagration wave.
  • the actively controllable neutron modifying structures 830 insert neutron absorbers into nuclear fission fuel within or to the side of the burnfront 810 , thereby changing the effective size of the burnfront 810 .
  • the actively controllable neutron modifying structures 830 insert neutron moderators, such as without limitation hydrocarbons or Li7, thereby modifying the neutron energy spectrum, and thereby changing the neutronic reactivity of nuclear fission fuel that is presently being burned by the burnfront 810 relative to neutronic reactivity of nuclear fission fuel ahead of or behind the burnfront 810 .
  • an effect of the neutron moderators is associated with detailed changes in the neutron energy spectrum (e.g., hitting or missing cross-section resonances), while in other cases the effects are associated with lowering the mean neutron energy of the neutron environment (e.g., downshifting from “fast” neutron energies to epithermal or thermal neutron energies).
  • an effect of the neutron moderators is to deflect neutrons to or away from selected locations.
  • one of the aforementioned effects of neutron moderators is of primary importance, while in other embodiments, multiple effects are of comparable design significance.
  • the actively controllable neutron modifying structures 830 contain both neutron absorbers and neutron moderators; in one nonlimiting example, the location of neutron absorbing material relative to that of neutron moderating material is changed to affect control (e.g., by masking or unmasking absorbers, or by spectral-shifting to increase or decrease the absorption of absorbers), in another nonlimiting example, control is affected by changing the amounts of neutron absorbing material and/or neutron moderating material.
  • the burnfront 810 can be directed as desired according to selected propagation parameters.
  • propagation parameters can include a propagation direction or orientation of the burnfront 810 , a propagation rate of the burnfront 810 , power demand parameters such the heat generation density, cross-sectional dimensions of a burning region through which the burnfront 810 is to the propagated (such as an axial or lateral dimension of the burning region relative to an axis of propagation of the burnfront 810 ), or the like.
  • the propagation parameters may be selected so as to control the spatial or temporal location of the burnfront 810 , so as to avoid failed or malfunctioning control elements (e.g., neutron modifying structures or thermostats), or the like.
  • a nuclear fission reactor can be controlled with programmable thermostats, thereby enabling the temperature of the reactor's fuel-charge to be varied over time responsive to changes in operating parameters.
  • Temperature profiles 940 are determined as a function of position through a fuel-charge of a nuclear fission reactor 900 .
  • An operating temperature profile 942 of operating temperatures throughout the nuclear fission reactor 900 is established responsive to a first set of operating parameters, such as predicted power draw, thermal creep of structural materials, etc. At other times, or in other circumstances, the operating parameters may be revised. To that end, a revised operating temperature profile 944 of revised operating temperatures throughout the nuclear fission reactor 900 is established.
  • the nuclear fission reactor 900 includes programmable temperature responsive neutron modifying structures 930 .
  • the programmable temperature responsive neutron modifying structures 930 (an example of which is described in detail later) introduce and remove neutron absorbing or neutron moderating material into and from the fuel-charge of a nuclear fission reactor 900 .
  • a nuclear fission deflagration wave burnfront 910 is initiated and propagated in a fuel-charge of the nuclear fission reactor 900 .
  • the programmable temperature responsive neutron modifying structures 930 introduce neutron absorbing or moderating material into the fuel-charge of the nuclear fission reactor 900 to lower operating temperature in the nuclear fission reactor 900 or remove neutron absorbing or moderating material from the fuel-charge of the nuclear fission reactor 900 in order to raise operating temperature of the nuclear fission reactor 900 .
  • operating temperature profiles are only one example of control parameters which can be used to determine the control settings of programmable temperature responsive neutron modifying structures 930 , which are in such cases responsive to the selected control parameters, not necessarily to the temperature.
  • control parameters which can be used to determine the control settings of programmable temperature responsive neutron modifying structures 930 include power levels, neutron levels, neutron spectrum, neutron absorption, fuel burnup levels, and the like.
  • the neutron modifying structures 930 are used to control fuel burnup levels to relatively low (e.g., ⁇ 50%) levels in order to achieve high-rate “breeding” of nuclear fission fuel for use in other nuclear fission reactors, or to enhance suitability of the burnt nuclear fission fuel for subsequent re-propagation of a nuclear fission deflagration wave in a propagating nuclear fission deflagration wave reactor.
  • relatively low e.g., ⁇ 50%
  • Different control parameters can be used at different times, or in different portions of the reactor.
  • neutron modifying methods discussed previously in the context of neutron modifying structures can also be utilized in programmable temperature responsive neutron modifying structures 930 , including without limitation, the use of neutron absorbers, neutron moderators, combinations of neutron absorbers and/or neutron moderators, variable geometry neutron modifiers, and the like.
  • material can be nuclearly processed.
  • nuclearly processable material 1020 that has a set of non-irradiated properties
  • a nuclear fission deflagration wave propagating burnfront 1030 is originated and propagated along a direction indicated by arrows 1040 as described above.
  • the material 1020 is placed in neutronic coupling with a region of maximized reactivity 1010 , that is the material is neutron irradiated, as the nuclear fission deflagration wave propagating burnfront 1030 propagates through or in the vicinity of the material 1020 , thereby irradiating the material 1020 and conferring upon the material 1020 a desired set of modified properties.
  • the neutron irradiation of material 1020 may be controlled by the duration and/or extent of the nuclear fission deflagration wave propagating burnfront 1030 .
  • the neutron irradiation of material 1020 may be controlled by control of the neutron environment (e.g., the neutron energy spectrum for Np237 processing) via neutron modifying structures.
  • the propagating nuclear fission deflagration wave reactor 1000 may be operated in a “safe” sub-critical manner, relying upon an external source of neutrons to sustain the propagating burnfront 1030 , while using a portion of the fission-generated neutrons for nuclear processing of the material 1020 .
  • the material 1020 may be present before nuclear fission ignition occurs within the propagating nuclear fission deflagration wave reactor 1000 , while in other embodiments the material 1020 may be added after nuclear fission ignition. In some embodiments, the material 1020 is removed from the propagating nuclear fission deflagration wave reactor 1000 , while in other embodiments it remains in place.
  • a nuclear fission deflagration wave propagating burnfront 1030 is initiated and propagated in a propagating nuclear fission deflagration wave reactor 1000 along a direction indicated by arrows 1040 .
  • Material 1050 having a set of non-irradiated properties is loaded into the propagating nuclear fission deflagration wave reactor 1000 .
  • the material 1050 in transported into physical proximity and neutronic coupling with a region of maximized reactivity as the nuclear fission deflagration wave propagating burnfront 1030 passes through the material 1050 .
  • the material 1050 remains in neutronic coupling for a sufficient time interval to convert the material 1050 into material 1056 having a desired set of modified properties.
  • the material 1056 may be physically transported out of the reactor 1000 as generally indicated at 1054 .
  • the removal 1054 can take place either during operation of the propagating nuclear fission deflagration wave reactor 1000 or afterward it has been “shut-off”, and can be performed in either a continuous, sequential, or batch process.
  • the nuclearly processed material 1056 may be subsequently used as nuclear fission fuel in another nuclear fission reactor, such as without limitation LWRs or propagating nuclear fission deflagration wave reactors.
  • the nuclearly processed material 1056 may be subsequently used within the nuclear fission ignitor of a propagating nuclear fission deflagration wave reactor.
  • thermal management may be adjusted to provide thermal control appropriate for any changes in operational parameters, as appropriate for the revised materials or structures.
  • temperature-driven neutron absorption can be used to control a nuclear fission reactor, thereby “engineering-in” an inherently-stable negative temperature coefficient of reactivity (aT).
  • a nuclear fission reactor 1100 is instrumented with temperature detectors 1110 , such as without limitation thermocouples.
  • the nuclear fission reactor 1100 suitably can be any type of fission reactor whatsoever.
  • the nuclear fission reactor 1100 can be a thermal neutron spectrum nuclear fission reactor or a fast neutron spectrum nuclear fission reactor, as desired for a particular application.
  • the temperature detectors detect local temperature in the nuclear fission reactor 1100 and generate a signal 1114 indicative of a detected local temperature.
  • the signal 1114 is transmitted to a control system 1120 in any acceptable manner, such as without limitation, fluid coupling, electrical coupling, optical coupling, radiofrequency transmission, acoustic coupling, magnetic coupling, or the like.
  • the control system 1120 determines an appropriate correction (positive or negative) to local neutronic reactivity in the nuclear fission reactor 1100 to return the nuclear fission reactor 1100 to desired operating parameters (such as desired local temperatures for full reactor power). To that end, the control system 1120 generates a control signal 1124 indicative of a desired correction to local neutronic reactivity.
  • the control signal 1124 is transmitted to a dispenser 1130 of neutron absorbing material.
  • the signal 1124 suitably is transmitted in the same manner as the signal 1114 .
  • the neutron absorbing material suitably is any neutron absorbing material as desired for a particular application, such as without limitation Li6, B10, or Gd.
  • the dispenser 1130 suitably is any reservoir and dispensing mechanism acceptable for a desired application, and may, for example, have the reservoir located remotely (e.g., outside the neutron reflector of the nuclear fission reactor 1100 ) from the dispensing mechanism 1130 .
  • the dispenser 1130 dispenses the neutron absorbing material within the nuclear fission reactor core responsive to the control signal 1124 , thereby altering the local neutronic reactivity.
  • exemplary thermal control may be established with a neutron absorbing fluid.
  • a thermally coupled fluid containing structure 1140 contains a fluid in thermal communication with a local region of the nuclear fission reactor 1100 .
  • the fluid in the structure 1140 expands or contracts responsive to local temperature fluctuations. Expansion and/or contraction of the fluid is operatively communicated to a force coupling structure 1150 , such as without limitation a piston, located external to the nuclear fission reactor 1100 .
  • a resultant force communicated by the force coupling structure 1150 is exerted on neutron absorbing fluid in a neutron absorbing fluid containing structure 1160 .
  • the neutron absorbing fluid is dispensed accordingly from the structure 1160 , thereby altering the local neutronic reactivity.
  • a neutron moderating fluid may be used instead of, or in addition to, the neutron absorbing fluid.
  • the neutron moderating fluid changes the neutron energy spectrum and lowers the mean neutron energy of the local neutron environment, thereby driving down or lowering neutronic reactivity of nuclear fission fuel within the nuclear fission reactor 1100 .
  • the neutron absorbing fluid and/or the neutron modifying fluid may have a multiple phase composition (e.g., solid pellets within a liquid).
  • FIG. 11C illustrates details of an exemplary implementation of the arrangement shown in FIG. 11B .
  • fuel power density in a nuclear fission reactor 1100 ′ is continuously regulated by the collective action of a distributed set of independently-acting thermostating modules, over very large variations in neutron flux, significant variations in neutron spectrum, large changes in fuel composition and order-of-magnitude changes in power demand on the reactor. This action provides a large negative temperature coefficient of reactivity just above the design-temperature of the nuclear fission reactor 1100 ′.
  • each of these modules includes a pair of compartments 1140 ′ and 1160 ′, each one of which is fed by a capillary tube.
  • the small thermostat-bulb compartment 1160 ′ located in the nuclear fission fuel contains a thermally sensitive material, such as without limitation, Li 7 , whose neutron absorption cross-section may be low for neutron energies of interest, while the relatively large compartment 1140 ′ positioned in a different location (e.g., on the wall of a coolant tube) may contain variable amounts of a neutron absorbing material, such as without limitation, Li 6 , which has a comparatively large neutron absorption cross-section.
  • Lithium melts at 453 K and 1-bar-boils at 1615 K, and therefore is a liquid across typical operating temperature ranges of the nuclear fission reactor 1100 ′.
  • the thermally sensitive material contained in the thermostat-bulb 1160 ′ expands, and a small fraction of it is expelled (approximately 10 ⁇ 3 , for a 100K temperature change in Li 7 ), potentially under kilobar pressure, into the capillary tube which terminates on the bottom of a cylinder-and-piston assembly 1150 ′ located remotely (e.g., outside of the radiation shield) and physically lower than the neutron absorbing material's intra-core compartment 1140 ′ (in the event that gravitational forces are to be utilized).
  • a cylinder-and-piston assembly 1150 ′ located remotely (e.g., outside of the radiation shield) and physically lower than the neutron absorbing material's intra-core compartment 1140 ′ (in the event that gravitational forces are to be utilized).
  • the modest volume of high-pressure thermally sensitive material drives a swept-volume-multiplying piston in the assembly 1150 ′ which pushes a potentially three order-of-magnitude larger volume of neutron absorbing material through a core-threading capillary tube into an intra-core compartment proximate to the thermostat-bulb which is driving the flow.
  • the neutron absorbing material whose spatial configuration is immaterial as long as its smallest dimension is less than a neutron mean free path, acts to absorptively depress the local neutron flux, thereby reducing the local fuel power density.
  • neutron absorbing material returns to the cylinder-and-piston assembly 1150 ′ (e.g., under action of a gravitational pressure-head), thereby returning the thermally sensitive material to the thermostat-bulb 1160 ′ whose now-lower thermomechanical pressure permits it to be received.
  • the thermally sensitive material may be chemically, not just isotopically, different from the neutron absorbing material.
  • the thermally sensitive material may be isotopically the same as the neutron absorbing material, with the differential neutron absorbing properties due to a difference in volume of neutronically exposed material, not a difference in material composition.
  • a propagating nuclear fission deflagration wave reactor 1200 operates at core temperatures significantly lower than core temperatures of nuclear fission reactors of other embodiments. While nuclear fission reactors of other embodiments may operate at core temperatures in the order of around 1,000K or so, (e.g., to enhance electrical power conversion efficiency) the propagating nuclear fission deflagration wave reactor 1200 operates at core temperatures of less than around 550K, and some embodiments operate at core temperatures of between around 400K and around 500K.
  • Reactor coolant 1210 transfers heat from nuclear fission in the propagating nuclear fission deflagration wave reactor 1200 . In turn thermal energy 1220 is transferred from the reactor coolant 1210 to a thermally driven application.
  • exemplary thermally driven applications include desalinating seawater, processing biomass into ethanol, space-heating, and the like.
  • a propagating nuclear fission deflagration wave reactor 1200 may operate at core temperatures above 550K, and utilize thermal energy 1220 from the reactor coolant 1210 for thermally driven applications instead of, or in addition to, electrical power generation applications.
  • exemplary thermally driven applications include thermolysis of water, thermal hydrocarbon processing, and the like.
  • nuclear fission fuel can be removed after it has been burned.
  • a nuclear fission deflagration wave propagating burnfront 1310 is initiated and propagated in a modular nuclear fission reactor core 1300 along a direction indicated by arrows 1320 toward modules 1340 of nuclear fission fuel material, thereby establishing a region 1330 of maximized reactivity as discussed above.
  • the modules 1340 of nuclear fission fuel material may be considered “burnt” after the propagating burnfront 1310 has propagated the region 1330 of maximized reactivity through the module 1340 of nuclear fission fuel material.
  • the modules 1340 of nuclear fission fuel material “behind” the region 1330 of maximized reactivity may be considered “burnt”. Any desired number of the “burnt” modules 1340 of nuclear fission fuel material (behind the region 1330 of maximized reactivity) are removed, as generally indicated at 1350 . As generally indicated at 1360 , nuclear fission fuel material has been removed from the nuclear fission reactor core 1300 .
  • the nuclear fission deflagration wave burnfront 1440 After the nuclear fission deflagration wave burnfront 1440 propagates into region 1420 , and either before or after it reaches an end of the propagating nuclear fission deflagration wave reactor 1400 , the nuclear fission deflagration wave burnfront 1440 is redirected or re-initiated and retraces a path of propagation away from the end of the propagating nuclear fission deflagration wave reactor 1400 back toward the region 1410 .
  • the nuclear fission deflagration wave burnfront 1440 propagates through the region 1410 as a nuclear fission deflagration wave burnfront 1450 away from the region 1420 toward an end of the propagating nuclear fission deflagration wave reactor 1400 .
  • the nuclear fission fuel in regions 1410 and 1420 is different during the repropagation of nuclear fission deflagration wave burnfronts 1440 and 1450 than it was during the previous propagation of nuclear fission deflagration wave burnfronts 1430 and 1440 , due to changes in the amounts of fissile isotopes and the amounts of fission product “ash”.
  • the neutron environment may differ during propagation and repropagation due to the above differences in the nuclear fission fuel, as well as other factors, such as without limitation, possible changes in the control of neutron modifying structures, thermal heat extraction levels, or the like.
  • the geometry of an embodiment of the propagating nuclear fission deflagration wave reactor 1400 forms a closed loop, such as an approximately toroidal shape.
  • the propagating nuclear fission deflagration wave reactor 1400 includes the regions 1410 and 1420 and a third region 1460 different from the regions 1410 and 1420 .
  • the nuclear fission deflagration wave burnfront 1430 is initiated and propagated through the region 1410 toward the region 1420 .
  • the nuclear fission deflagration wave burnfront 1430 propagates through the region 1420 as the nuclear fission deflagration wave burnfront 1440 .
  • the nuclear fission deflagration wave burnfront 1440 propagates through the region 1460 as a nuclear fission deflagration wave burnfront 1470 .
  • nuclear fission fuel material in the regions 1410 , 1420 , and 1460 can be considered “burnt”.
  • the nuclear fission deflagration wave burnfront 1430 is re-initiated and propagates through the region 1410 as a nuclear fission deflagration wave burnfront 1450 .
  • the re-initiation in region 1410 may occur without limitation, through the action of a nuclear fission igniter, such as discussed earlier, or may occur as a result of the decay and/or removal of nuclear fission products from the nuclear fission fuel material in region 1410 , or may occur as the result of other sources of neutrons or fissile material, or may occur due to control of neutron modifying structures, as discussed previously.
  • the nuclear fission deflagration wave may potentially propagate in a plurality of directions.
  • One or more propagation paths may be established, and may thereafter split into one or more separate propagation paths.
  • the splitting of propagation paths may be accomplished without limitation by such methods as the configuration of the nuclear fission fuel material, the action of neutron modifying structures as discussed earlier, or the like.
  • Propagation paths may be distinct, or may be reentrant.
  • Nuclear fission fuel material may be burnt once, never, or multiple times. Repropagation of a nuclear fission deflagration wave multiple times through a region of nuclear fission fuel material may involve either the same or a different propagation direction.
  • nuclear fission fuel cores of nonuniform material may be used.
  • nuclear fission fuel cores may include regions having different percentages of uranium and thorium.
  • nuclear fission fuel cores may include regions of different actinide or transuranic isotopes, such as without limitation different isotopes of thorium or different isotopes of uranium.
  • mixtures of such different combinations may also be appropriate.
  • mixtures of thorium and of different uranium isotope ratios may provide different burning rates, temperatures, propagation features, localization, or other features.
  • the nuclear fission fuel cores may include mixtures of “breedable” isotopes (such as Th232 or U238) along with other fissionable actinide or transuranic elements, such as without limitation, uranium, plutonium, americium, or the like.
  • variations in chemicals, isotopes, cross sections, densities, or other aspects of the fuel may vary radially, axially or in a variety of other spatial manners.
  • such variations may be defined according to anticipated variations in energy demand, aging, or other anticipated variations. In one aspect, where growth of energy demand in a region would be reasonably anticipated, it may be useful to define the fuel or materials to correlate to an expected increased demand of the region.
  • such variations may be implemented according to other approaches described herein.
  • the variations may be defined after initiation of burning using the modular approach is described herein or the multipath approaches described herein.
  • movement of portions of the material may produce the appropriate material concentrations, positioning, ratios, or other characteristics.
  • propagating nuclear fission deflagration wavefronts may remain substantially spatially fixed while the fuel core or portions of the fuel core move relative to the wavefront.
  • movement of the nuclear fission fuel core to maintain substantially localized positioning of the propagating nuclear fission deflagration wavefront can stabilize, optimize, or otherwise control thermal coupling to a cooling or heat transfer system.
  • controlled positioning of the propagating nuclear fission deflagration wavefront by physically displacing the nuclear fission fuel can simplify or reduce constraints upon other aspects of the nuclear fission reactor, such as the cooling system, neutron shielding, or other aspects of neutron density control.

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US11/605,933 US20080123795A1 (en) 2006-11-28 2006-11-28 Controllable long term operation of a nuclear reactor
KR1020097013475A KR20090085145A (ko) 2006-11-28 2007-11-26 원자로를 장기간 제어 운전하는 방법
CA002670919A CA2670919A1 (en) 2006-11-28 2007-11-26 Controllable long term operation of a nuclear reactor
JP2009539275A JP2010511173A (ja) 2006-11-28 2007-11-26 原子炉の制御可能な長期運転
EP07873828A EP2097906A4 (en) 2006-11-28 2007-11-26 CONTROLLABLE LONG-TERM OPERATION OF A CORE REACTOR
CN200780049972.8A CN101589439B (zh) 2006-11-28 2007-11-26 核反应堆的可控制的长期运行
PCT/US2007/024375 WO2008105856A2 (en) 2006-11-28 2007-11-26 Controllable long term operation of a nuclear reactor
US12/069,908 US9230695B2 (en) 2006-11-28 2008-02-12 Nuclear fission igniter
US12/069,907 US9275759B2 (en) 2006-11-28 2008-02-12 Modular nuclear fission reactor
US12/157,714 US20090080587A1 (en) 2006-11-28 2008-06-11 Nuclear fission igniter
US12/157,720 US20090080588A1 (en) 2006-11-28 2008-06-11 Nuclear fission igniter
US12/316,446 US9831004B2 (en) 2006-11-28 2008-12-12 Controllable long term operation of a nuclear reactor
JP2013079884A JP6026944B2 (ja) 2006-11-28 2013-04-05 原子炉の制御可能な長期運転
US14/251,894 US9305669B2 (en) 2006-11-28 2014-04-14 Controllable long term operation of a nuclear reactor
US15/791,923 US10706979B2 (en) 2006-11-28 2017-10-24 Controlling spatial position of a propagating nuclear fission deflagration wave within a burning wavefront heat generating region

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CA2670919A1 (en) 2008-09-04
WO2008105856A2 (en) 2008-09-04
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JP2013178253A (ja) 2013-09-09
KR20090085145A (ko) 2009-08-06
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WO2008105856A3 (en) 2009-01-08
CN101589439A (zh) 2009-11-25

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