nuclear ceramics, ceramic materials employed in the generation of nuclear power and in the disposal of radioactive nuclear wastes.

In their nuclear-related functions, ceramics are of major importance. Since the beginning of nuclear power generation, oxide ceramics, based on the fissionable metals uranium and plutonium, have been made into highly reliable fuel pellets for both water-cooled and liquid-metal-cooled reactors. Ceramics also can be employed to immobilize and store nuclear wastes. Although vitrification (glass formation) is a favoured approach for waste disposal, wastes can be processed with other ceramics into a synthetic rock, or synroc, or they can be mixed with cement powder to make hardened cements. All these nuclear applications are extremely demanding. In addition to severe thermal and chemical driving forces, nuclear ceramics are continuously subjected to high radiation doses.

This article describes properties and applications of ceramics as nuclear fuels and as waste-disposal materials. For discussion of the employment of glassy and metallic materials in nuclear waste disposal, see materials science: Materials for energy. For the production of metallic uranium and plutonium and their conversion to oxide form, see uranium processing. For detailed description of nuclear reactors and the nuclear fuel cycle, see nuclear reactor.

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Nuclear fuel

Ceramic oxide fuels were introduced in the 1950s, following military applications of nuclear power. Urania (uranium dioxide, UO2) and plutonia (plutonium dioxide, PuO2) have unique features that qualify them for nuclear fuel applications. First, they are extremely refractory: for instance, the melting point of UO2 is in excess of 2,800° C (5,100° F). Second, the open crystal structure of oxide nuclear ceramics allows for retention of fission products, and their highly variable oxygen-to-metal ratio can shift to accommodate burnup. They therefore have excellent resistance to radiation damage. (The crystal structure of urania is illustrated in Figure 2B of the article ceramic composition and properties: Crystal structure.)

Other advantages of oxide nuclear fuels include inertness to many coolants, long burnup without swelling, and relatively low fabrication cost. One drawback is low thermal conductivity. This has prompted research on replacing the oxides with more conductive carbides or nitrides. Selected properties of oxide, carbide, and nitride nuclear fuels are compared in Table 1.

Selected properties of ceramic nuclear fuels*
ceramic fuel density (gm/cm3) thermal conductivity (W • m−1 • K−1)** melting point (°C)
*Reprinted from H. Tsai, "Carbide and Nitride Nuclear Fuels," in Michael B. Bever (ed.), Encyclopedia of Materials Science and Engineering (1986), pp. 493–495, with permission from Elsevier Science.
**At approximately 1,000 °C.
urania (UO2) 10.97 2.8 2,847
urania/plutonia (UO2/PuO2) 11.06 2.8 2,787
uranium carbide (UC) 13.51 21.7 2,507
uranium nitride (UN) 14.32 24.5 2,762

The fabrication of ceramic nuclear fuels traditionally follows a standard powder-pellet process. This involves comminution, granulation, pressing, and sintering at 1,700° C (3,100° F) in a reducing atmosphere. The resulting microstructure consists of large, equiaxed grains (that is, with dimensions similar along all axes), with uniformly distributed spherical pores on the order of 2 to 5 micrometres (0.00008 to 0.0002 inch). The pores are intended to retain fission gas and to decrease swelling during burnup.

Ceramic fuel pellets also can be fabricated in an advanced process called sol-gel microsphere pelletization. The sol-gel route (described in the article advanced ceramics) achieves homogeneous distribution of uranium and plutonium in solid solution, enables sintering to occur at lower temperature, and ameliorates the toxic dust problem associated with the powder-pellet method.

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Nuclear waste disposal

High-level waste

A 1,000-megawatt nuclear power reactor produces on the order of 20–25 tons of spent fuel per year. Spent fuel is initially stored for up to several decades underwater in storage pools. This allows the high-activity, short-half-life radioactivity to decay. Some of this material can be reprocessed to recover reusable uranium and plutonium. However, the waste also contains radioactive isotopes with much longer half-lives. It is widely accepted that this high-level waste (HLW) must be incorporated into a solid form prior to burial in deep geologic repositories.

The requirements of a nuclear waste form for HLW are rigorous. The waste form must be able to take into solid solution or at least to encapsulate the radioactive species. This is necessary so that the rate of leaching into underground water in a geologic repository will be acceptably low. Leach resistance must be maintained against deterioration of the waste form by radiation damage over long time periods, possibly lasting thousands of years. The form must be amenable to fabrication into large cylindrical monoliths, approximately 30 centimetres (1 foot) in diameter, with minimal internal cracking. Other important considerations are low cost and personnel safety from such hazards as respirable dust and radiation exposure.

In most nuclear countries the accepted first-generation solid form for disposing of HLW is borosilicate glass. In borosilicate forms, some radioactive species become part of the glass structure and others are merely encapsulated. The most advanced second-generation solid waste form is synroc, a ceramic synthetic rock. Synroc contains various titanate-mineral phases that have the capability of forming solid solutions with nearly all the radioactive species in HLW. Similar minerals exist in nature, where they have survived under demanding conditions for geologic time periods. The production of synroc involves mixing oxides or appropriate alkoxides with HLW, drying and calcining under reducing conditions, and hot-pressing or hot-isostatic-pressing the powder in graphite or refractory metal dies. (Hot pressing and hot isostatic pressing are described in the article advanced ceramics.)

Low-level waste

Over the years low-level wastes (LLW) have accumulated from the processing of nuclear fuels and wastes. These consist of aqueous solutions and sludges, which customarily have been stored in steel-lined underground tanks. However, concerns over actual and potential leaks from these tanks leading to groundwater contamination have prompted the development of solid waste forms for LLW. Some of this material will be glassy, but one promising route is to make cement with the aqueous LLW. Immobilization of some radioactive species would take place by chemical incorporation into the cementitious product phases; the rest would be immobilized within the pores of the cement paste. Extremely low permeabilities (and therefore low leach rates) can be achieved in microstructurally engineered cements.

Nuclear ceramics are only one type of advanced structural ceramic. For a survey of the issues involved in adapting ceramics for demanding structural applications, see advanced structural ceramics. For a directory to all the articles covering both traditional and advanced industrial ceramics, see Industrial Ceramics: Outline of Coverage.

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Taiwan Shuts Last Nuclear Reactor as Energy Debate Heats Up May 16, 2025, 10:56 PM ET (Bloomberg)

nuclear reactor, any of a class of devices that can initiate and control a self-sustaining series of nuclear fissions. Nuclear reactors are used as research tools, as systems for producing radioactive isotopes, and most prominently as energy sources for nuclear power plants.

Principles of operation

Nuclear reactors operate on the principle of nuclear fission, the process in which a heavy atomic nucleus splits into two smaller fragments. The nuclear fragments are in very excited states and emit neutrons, other subatomic particles, and photons. The emitted neutrons may then cause new fissions, which in turn yield more neutrons, and so forth. Such a continuous self-sustaining series of fissions constitutes a fission chain reaction. A large amount of energy is released in this process, and this energy is the basis of nuclear power systems.

In an atomic bomb the chain reaction is designed to increase in intensity until much of the material has fissioned. This increase is very rapid and produces the extremely prompt, tremendously energetic explosions characteristic of such bombs. In a nuclear reactor the chain reaction is maintained at a controlled, nearly constant level. Nuclear reactors are so designed that they cannot explode like atomic bombs.

Most of the energy of fission—approximately 85 percent of it—is released within a very short time after the process has occurred. The remainder of the energy produced as a result of a fission event comes from the radioactive decay of fission products, which are fission fragments after they have emitted neutrons. Radioactive decay is the process by which an atom reaches a more stable state; the decay process continues even after fissioning has ceased, and its energy must be dealt with in any proper reactor design.

Chain reaction and criticality

The course of a chain reaction is determined by the probability that a neutron released in fission will cause a subsequent fission. If the neutron population in a reactor decreases over a given period of time, the rate of fission will decrease and ultimately drop to zero. In this case the reactor will be in what is known as a subcritical state. If over the course of time the neutron population is sustained at a constant rate, the fission rate will remain steady, and the reactor will be in what is called a critical state. Finally, if the neutron population increases over time, the fission rate and power will increase, and the reactor will be in a supercritical state.

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Before a reactor is started up, the neutron population is near zero. During reactor start-up, operators remove control rods from the core in order to promote fissioning in the reactor core, effectively putting the reactor temporarily into a supercritical state. When the reactor approaches its nominal power level, the operators partially reinsert the control rods, balancing out the neutron population over time. At this point the reactor is maintained in a critical state, or what is known as steady-state operation. When a reactor is to be shut down, operators fully insert the control rods, inhibiting fission from occurring and forcing the reactor to go into a subcritical state.

Reactor control

A commonly used parameter in the nuclear industry is reactivity, which is a measure of the state of a reactor in relation to where it would be if it were in a critical state. Reactivity is positive when a reactor is supercritical, zero at criticality, and negative when the reactor is subcritical. Reactivity may be controlled in various ways: by adding or removing fuel, by altering the ratio of neutrons that leak out of the system to those that are kept in the system, or by changing the amount of absorber that competes with the fuel for neutrons. In the latter method the neutron population in the reactor is controlled by varying the absorbers, which are commonly in the form of movable control rods (though in a less commonly used design, operators can change the concentration of absorber in the reactor coolant). Changes of neutron leakage, on the other hand, are often automatic. For example, an increase of power will cause a reactor’s coolant to reduce in density and possibly boil. This decrease in coolant density will increase neutron leakage out of the system and thus reduce reactivity—a process known as negative-reactivity feedback. Neutron leakage and other mechanisms of negative-reactivity feedback are vital aspects of safe reactor design.

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A typical fission interaction takes place on the order of one picosecond (10−12 second). This extremely fast rate does not allow enough time for a reactor operator to observe the system’s state and respond appropriately. Fortunately, reactor control is aided by the presence of so-called delayed neutrons, which are neutrons emitted by fission products some time after fission has occurred. The concentration of delayed neutrons at any one time (more commonly referred to as the effective delayed neutron fraction) is less than 1 percent of all neutrons in the reactor. However, even this small percentage is sufficient to facilitate the monitoring and control of changes in the system and to regulate an operating reactor safely.