An active zone includes a homogeneous uranium-plutonium nitride fuel, the mass fraction of which is a minimum 0.305, and consists of central, intermediate and peripheral parts which form fuel assemblies comprising fuel elements with geometrically identical shells but differing heights. The radial distribution of the fuel across the volume of the active zone has a stepped shape. The radius of the central part is from 0.4 to 0.5 of the effective active zone radius, while the height of the fuel column in the fuel elements in the central part is from 0.5 to 0.8 of the height of the fuel column in the peripheral part. The heights of the fuel columns forming a stepped intermediate part for diameters ranging from 0.5 to 0.85 of the effective active zone diameter are within the range from 0.55 to 0.9 of the height of the fuel column in the peripheral part.

A fabrication method of burnable absorber nuclear fuel pellets and burnable absorber nuclear fuel pellets fabricated by the same are provided, in which the fabrication method includes adding boron compound and manganese compound to one or more type of nuclear fuel powders selected from the group consisting of uranium dioxide (UO.sub.2), plutonium dioxide (PuO.sub.2) and thorium dioxide (ThO.sub.2) and mixing the same (step 1), compacting the mixed powder of step 1 into compacts (step 2), and sintering the compacts of step 2 under hydrogen atmosphere (step 3). According to the fabrication method, sintering can be performed under hydrogen atmosphere at a temperature lower than the hydrogen atmosphere sintering that is conventionally applied in the nuclear fuel sintered pellet mass production, by adding sintering additives such as manganese oxide or the like.

A nanofuel engine including an inventive nanofuel internal engine, whereby nuclear energy is released in the working fluid and directly converted into useful work, with the qualities of an economical advanced small modular gaseous pulsed thermal reactor. Scientific feasibility is established by studying the behavior of nuclear fuels in configurations designed to support a fission chain reaction. Nanofuel is defined as nuclear fuel suitable for use in an internal engine, comprised of six essential ingredients, and can be created from clean fuel or from the transuranic elements found in light-water reactor spent nuclear fuel in a proliferation resistant manner. Three essential ingredients ensure the nanofuel is inherently stable, due to a negative temperature coefficient of reactivity. Reciprocating and Wankel (rotary) internal engine configurations, which operate in an Otto cycle, are adapted to support a fission chain reaction. Dynamic engine cores experience a decrease in criticality as the engine piston or rotor moves away from the top dead center position. In this inherent safety feature, the increase in engine core volume decreases the nanofuel density and increases the neutron leakage. Technological feasibility is demonstrated by examining potential engineering limitations. The nanofuel internal engine can be operated in two modes: spark-ignition with an external neutron source such as a fusion neutron generator; and compression-ignition with an internal neutron source. The structural integrity can be maintained using standard internal combustion engine design and operation practices. The fuel system can be operated in a closed thermodynamic cycle, which allows for complete fuel utilization, continuous refueling, and easy fission product extraction. Nanofuel engine power plant configurations offer favorable economic, safety, and waste management attributes when compared to existing power generation technology. The initial (first-of-a-kind) overnight capital cost is approximately $400 per kilowatt-electric. Obvious safety features include an underground installation, autonomous operation, and an ultra-low nuclear material inventory.

A fuel element has a ratio of area of fissionable nuclear fuel in a cross-section of the tubular fuel element perpendicular to the longitudinal axis to total area of the interior volume in the cross-section of the tubular fuel element that varies with position along the longitudinal axis. The ratio can vary with position along the longitudinal axis between a minimum of 0.30 and a maximum of 1.0. Increasing the ratio above and below the peak burn-up location associated with conventional systems reduces the peak burn-up and flattens and shifts the burn-up distribution, which is preferably Gaussian. The longitudinal variation can be implemented in fuel assemblies using fuel bodies, such as pellets, rods or annuli, or fuel in the form of metal sponge and meaningfully increases efficiency of fuel utilization.

A fast neutron nuclear reactor contains a nuclear reactor core having an array of device locations. Some device locations in the nuclear reactor core contain fissile and fertile nuclear fuel assembly devices. One or more other device locations in the nuclear reactor core contain Doppler reactivity augmentation devices that amplify the negativity of the Doppler reactivity coefficient within the nuclear reactor core. In some implementations, a Doppler reactivity augmentation device can also reduce the coolant temperature coefficient within the nuclear reactor core. Accordingly, a Doppler reactivity augmentation device contributes to a more stable nuclear reactor core.

Fissile target materials are provided. The fissile target materials can include a target substrate and a capturing layer operably interfacing with at least one surface of the target substrate. Fission fissile target materials are also provided that can include a target substrate comprising at least one fissile atom and a capturing layer operably interfacing with at least one surface of the target substrate. The capturing layer can include at least one fission product.

Fissile target materials are provided. The fissile target materials can include a target substrate and a capturing layer operably interfacing with at least one surface of the target substrate. Fission fissile target materials are also provided that can include a target substrate comprising at least one fissile atom and a capturing layer operably interfacing with at least one surface of the target substrate. The capturing layer can include at least one fission product.