Dispersion ceramic micro-encapsulated (DCM) nuclear fuel and related methods
09620248 ยท 2017-04-11
Assignee
Inventors
Cpc classification
G21C3/26
PHYSICS
G21C3/20
PHYSICS
G21C3/17
PHYSICS
G21C21/02
PHYSICS
Y02E30/30
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
C04B2237/74
CHEMISTRY; METALLURGY
International classification
Abstract
The invention relates to the use of Dispersion Ceramic Micro-Encapsulated (DCM) nuclear fuel as a meltdown-proof, accident-tolerant fuel to replace uranium dioxide fuel in existing light water reactors (LWRs). The safety qualities of the DCM fuel are obtained by the combination of three strong barriers to fission product release (ceramic coatings around the fuel kernels), highly dense inert ceramic matrix around the coated fuel particles and metallic or ceramic cladding around the fuel pellets.
Claims
1. A nuclear fuel comprising: a dispersion-ceramic micro-encapsulated fuel comprising a plurality of tristructural-isotropic (TRISO) fuel particles embedded in a silicon carbide matrix; wherein the plurality of TRISO fuel particles each include one or more layers of isotropic materials surrounding a fuel kernel and the fuel kernel is surrounded by a porous carbon buffer layer, an inner pyrolytic carbon layer, a ceramic layer, and an outer pyrolytic carbon layer; wherein the ceramic layer is formed of a silicon carbide layer supplemented with a zirconium carbide; and wherein the plurality of TRISO fuel particles includes two or more different sizes of TRISO fuel particles, including a first TRISO fuel particle having a first fuel kernel with a first kernel radius of no more than 375 micrometers and a first packing fraction of no more than 45% and a second TRISO fuel particle having a second fuel kernel with a second kernel radius of no more than 200 micrometers and a second packing fraction of no more than 3%.
2. The nuclear fuel of claim 1, wherein the dispersion-ceramic micro-encapsulated fuel is comprised of heavy metal materials providing higher density than uranium dioxide.
3. The nuclear fuel of claim 2, wherein the heavy metal materials are selected from a group consisting of uranium nitride, uranium carbide, and uranium silicide.
4. The nuclear fuel of claim 3, wherein the fuel includes resonant absorbers selected from a group consisting of gadolinium or erbium.
5. The nuclear fuel of claim 1, wherein the silicon carbide matrix comprises silicon carbide powder mixed with sintering additives.
6. The nuclear fuel of claim 1, wherein the fuel kernel includes a fissile material and a fertile material in an oxide, carbide, or oxycarbide form.
7. The nuclear fuel of claim 6, wherein the fertile material is selected from a group consisting of uranium, plutonium, or thorium.
8. The nuclear fuel of claim 1, wherein the fuel kernel comprises low enriched uranium.
9. The nuclear fuel of claim 1, wherein the porous carbon buffer layer surrounds the fuel kernel and is a reservoir for accommodating buildup of fission gases diffusing out of the fuel kernel and mechanical deformation that the fuel kernel undergoes during a fuel cycle.
10. The nuclear fuel of claim 1, wherein the ceramic layer is formed of silicon carbide material.
11. The nuclear fuel of claim 1, wherein the first TRISO fuel particle has a pellet radius between 0.4095 and 0.4709 centimeters and a pellet height of 1 centimeter.
12. The nuclear fuel of claim 11, wherein: the porous carbon buffer layer of the first TRISO fuel particle has a porous carbon buffer layer radius of 0.0475 centimeters; the inner pyrolytic carbon layer of the first TRISO fuel particle has an inner pyrolytic carbon radius of 0.0510 centimeters; the ceramic layer of the first TRISO fuel particle has a ceramic layer radius of 0.0545 centimeters; and the outer pyrolytic carbon layer of the first TRISO fuel particle has an outer pyrolytic carbon layer radius of 0.0585 centimeters.
13. The nuclear fuel of claim 12, wherein the second TRISO fuel particle has a pellet radius of 0.4709 centimeters and a pellet height of 1 centimeter.
14. The nuclear fuel of claim 13, wherein: the porous carbon buffer layer radius of the second TRISO fuel particle is 0.0300 centimeters; the inner pyrolytic carbon layer radius of the second TRISO fuel particle is 0.0335 centimeters; the ceramic layer radius of the second TRISO fuel particle is 0.0370 centimeters; and the outer pyrolytic carbon layer radius is 0.0410 centimeters.
15. The nuclear fuel of claim 14, wherein the fuel kernel comprises uranium nitride.
16. The nuclear fuel of claim 14, wherein the fuel kernel comprises uranium carbide.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) The accompanying drawings, which are incorporated in and constitute a part of this specification, illustrate several embodiments of the inventions and together with the description, serve to explain the principles of the inventions. The patent or application file contains at least one drawing executed in color. Copies of this patent or patent application publication with color drawing(s) will be provided by the Office upon request and payment of the necessary fee.
(2)
(3)
(4)
(5)
(6)
(7)
(8)
(9)
(10)
(11)
(12)
(13)
(14)
(15)
DESCRIPTION OF THE EMBODIMENTS
(16) Reference will now be made in detail to the exemplary embodiments consistent with the present inventions, examples of which are illustrated in the accompanying drawings. Wherever possible, the same reference characters will be used throughout the drawings to refer to the same or like parts.
(17) Dispersion fuels consist of a distribution of discrete fuel particles embedded in a non-fuel matrix. Ideally, the matrix remains largely not affected by neutron and fission fragment damage from the fission events that take place in the fuel particles.
(18) The best composite fuel uses fully encapsulated coated fuel particles embedded in an inert heat-conductive matrix and surrounded by a metallic or ceramic clad. In a well-designed dispersion fuel, there are three very strong barriers to fission product release to the coolant. These are the coating around the particle, the dense matrix, and the cladding around the dispersion fuel block, each of them independently capable of containing the fission products and chemically inactive.
(19) Given the available irradiation behavior database, the concept most likely to minimize fission gas release to the coolant will incorporate buffered particles in a dense matrix. This buffer material serves the dual role of providing volume for fission gas and providing volume for fuel particle swelling. The buffer layer is protected by a dense coating layer, also designed to provide for fission product retention. These are essentially TRISO coated fuel particles.
(20) TRISO fuel is a type of micro fuel particle that can be used effectively as the discrete fuel particles of a dispersion fuel concept. The term TRISO, as used herein, may refer to any type of micro fuel particle consisting of a fuel kernel composed of UC or uranium oxycarbide (UCO) in the center, coated with one or more layers surrounding one or more isotropic materials. In one preferred embodiment, TRISO particles include four layers of three isotropic materials. In that embodiment, the four layers are a porous buffer layer made of carbon, followed by a dense inner layer of pyrolytic carbon (PyC), followed by a ceramic layer of SiC to retain fission products at elevated temperatures and to give the TRISO particle a strong structural integrity, followed by a dense outer layer of PyC. TRISO fuel particles are designed not to crack due to the stresses or fission gas pressure at temperatures beyond 1600 C., and therefore can contain the fuel in the worst of accident scenarios. TRISO fuel was designed for use in high temperature gas cooled reactors, to be operating at temperatures much higher than the temperatures of LWRs.
(21) Of the possible matrix materials, silicon carbide (SiC) offers the largest existing database in terms of material properties, irradiation behavior, and fabrication. SiC has excellent oxidation resistance due to rapid formation of a dense, adherent silicon dioxide (SiO.sub.2) surface scale on exposure to air at elevated temperature, which prevents further oxidation. The low irradiation swelling behavior of SiC is well documented. Processing of SiC into dense shapes is currently done on an industrial scale at a reasonable cost, although major modifications will be required for processing of particle fueled composites.
(22) The use of coated particles makes it more difficult to achieve high heavy metal density in the fuel, since the net heavy metal density within a fuel particle falls rapidly with increasing coating thickness. This fact requires that the coating thickness to kernel diameter ratio be kept as small as possible while maintaining utility as a fission product barrier. It is however clear that the use of dispersion fuels in LWRs will demand higher enrichment and a lower power density. The most likely fissile particle types for composite fuels are uranium/plutonium carbides (UC or PuC) and uranium/plutonium nitrides (UN or PuN) due to the combination of high melting temperature and high actinide density. Uranium silicides could provide an even higher density of fissile uranium, but may be unstable under the expected fabrication and operation conditions.
(23) The dispersion fuel consisting of the combination of TRISO fuel particles and silicon carbide matrix in a ceramic cladding is known as dispersion ceramic micro-encapsulated (DCM) fuel.
(24) DCM fuel consists of UN or UC TRISO particles that are embedded inside a SiC matrix. This fuel design differs significantly from the previous dispersion type fuel approaches, since the damage due to 100 MeV fission fragments and noble gas release is fully contained within the TRISO particle and the inert SiC matrix is solely exposed to neutron irradiation. In addition to offering exceptional stability under neutron irradiation conditions (less than 1% swelling) the thermal conductivity of the SiC matrix is on the order of about 10 times higher than that of uranium dioxide. The fuel development and qualification process for DCM fuel has benefited from and will significantly be facilitated by decades of gas reactor TRISO fuel development and optimization activities.
(25)
(26) Referring to
(27) While the fuel element 10 of
(28) The fuel particles 20 dispersed in the SiC matrix 15 may be tristructuralisotropic (TRISO) fuel particles. The term TRISO fuel particle, as used herein, may refer to any type of micro fuel particle comprising a fuel kernel and one or more layers of isotropic materials surrounding the fuel kernel. By way of example only, the fuel particle 20 may have a diameter of about 1 millimeter.
(29) As shown in
(30) The fuel kernel 25 may be coated with four distinct layers: (1) a porous carbon buffer layer 22; (2) an inner pyrolytic carbon (PyC) layer 24; (3) the ceramic layer 26; and (4) an outer pyrolytic carbon (PyC) layer 28.
(31) The modeled behavior of DCM fuel is illustrated in
(32) As shown in
(33) The porous carbon buffer layer 22 surrounds the fuel kernel 25 and serves as a reservoir for accommodating buildup of fission gases diffusing out of the fuel kernel 25 and any mechanical deformation that the fuel kernel 25 may undergo during the fuel cycle.
(34) The inner PyC layer 24 may be formed of relatively dense PyC and seals the carbon buffer layer 22.
(35) The ceramic layer 26 may be formed of a SiC material and serve as a primary fission product barrier and a pressure vessel for the fuel kernel 25, retaining gaseous and metallic fission products therein. The ceramic layer 26 also provides overall structural integrity of the fuel particle 20.
(36) In some exemplary embodiments, the SiC layer 26 may be replaced or supplemented with zirconium carbide (ZrC) or any other suitable material having similar properties as those of SiC and/or ZrC.
(37) The outer PyC layer 28 protects the SiC layer 26 from chemical attack during operation and acts as an additional diffusion boundary to the fission products. The outer PyC layer 28 may also serve as a substrate for bonding to the surrounding matrix material.
(38) The configuration and/or composition of the fuel particle are not limited to the embodiments described above. Instead, it should be understood that a fuel particle consistent with the present disclosure may include one or more additional layers, or omit one or more layers, depending on the desired properties of the fuel particle. For example, the fuel particle 20 may be overcoated with the SiC matrix material (i.e., SiC layer) prior to being mixed and compressed with the SiC powder.
(39) An exemplary method of fabricating the fuel element 10, according to another aspect of the present inventions, will be described herein.
(40) To form the fuel particles 20, according to one exemplary embodiment, the material for the fuel kernel 25 may be dissolved in a nitric acid to form a solution (e.g., uranyl nitrate). The solution is then dropped through a small nozzle or orifice to form droplets or microspheres. The dropped microspheres are then gelled and calcined at high temperature to produce the fuel kernels 25. The fuel kernels 25 may then be run through a suitable coating chamber, such as a CVD furnace, in which desired layers are sequentially coated onto the fuel kernels 25 with high precision. It should be understood that any other fabrication method known in the art may be additionally or alternatively used to form the fuel kernels 25.
(41) Once the fuel particles 20 are prepared, the fuel particles 20 are mixed with SiC powder, which comprises the precursor for the SiC matrix 15. Prior to the mixing, the fuel particles 20 may be coated with a suitable surface protection material. The SiC powder may have an average size of less than 1 m and/or a specific surface area greater than 20 m.sup.2/g. By way of example only, the size of the SiC powder may range from about 15 nm to about 51 nm with the mean particle size being about 35 nm.
(42) During or prior to mixing, sintering additives, such as, for example, alumina and rare earth oxides, may be added to the SiC powder and/or coated onto the SiC powder surface. In one exemplary embodiment, the amount of additives may range from about 1 weight % to 10 weight %. When mixing with the fuel particles 20, the SiC-based precursor material containing the SiC powder may be in a variety of physical states (e.g., powder, liquid, slurry, etc.) depending on the mixing and/or fabrication method used.
(43) The SiC-based precursor mixed with the fuel particles 20 may then be pressed to stress at a predetermined pressure and temperature to form the fuel element 10. According to one exemplary embodiment, the sintering pressure and temperature during the press may be less than about 30 MPa and 1900 C., respectively. Preferably, the sintering pressure and temperature may be about 10 MPa and 1850 C., respectively. The duration of the press may be less than or equal to about one hour, but it may take more than one hour.
(44) The small size or large specific surface area of the SiC powder, with the limited mass fraction of the sintering additives, may enable the formation of highly crystalline, near-full density, SiC matrix at conditions sufficient to ensure the integrity of the fuel particles 20. The SiC matrix provides an additional barrier to fission products that may be released during normal operation and accident temperatures and contaminate the coolant of the reactor. The SiC matrix also helps contain fission products after disposal.
(45) For example,
(46) In addition, the SiC matrix 15 has very low permeability to helium (e.g., in the order of about 10.sub.10 to 10.sub.11 m.sub.2/s), which is substantially lower than that of graphite and makes it particularly suitable for a gas cooled reactor that uses helium as a coolant. Low permeability of the SiC matrix 15 may also ensure retention of fission product gas.
(47)
(48) For example, higher thermal conductivity may permit operating the nuclear reactor at higher temperature. Operating a reactor at higher temperature may increase the efficiency and the power density, which may permit reduction of the reactor size. Higher thermal conductivity may also permit higher burnup of the fuel element while maintaining the overall fuel integrity. Moreover, as briefly mentioned above, higher burnup may not only reduce the overall waste volume but also limit possible nuclear proliferation and diversion opportunities. Furthermore, fuel with high thermal conductivity may undergo less severe temperature transients during an accident condition, such as a loss of coolant accident (LOCA). In light water reactor operating conditions, migration of fission products (including gases) outside the TRISO fuel particles and the SiC matrix is not expected to occur.
(49) Further, the SiC matrix 15 has higher fracture strength, higher irradiation resistance, and lower irradiation swelling than graphite or UO.sub.2. The combination of better irradiation performance and better thermal conductivity may result in better mechanical performance as compared to graphite or UO.sub.2 fuel element. The resulting matrix 15 is considered a near-stoichiometric, radiation-resistant, form of SiC, allowing the fuel element 10 to be repository-stable for direct disposal even after substantial burnup (e.g., 6099% burnup).
(50) Now, with reference to
(51) In one exemplary embodiment, one or more fuel elements 10 may be enclosed in a metallic cladding tube 35 or any other suitable enclosure to form a fuel rod 30, as shown in
(52) According to another aspect of the present inventions, the fuel element may be provided as an elongated rod fuel element 100, as shown in
(53) Other embodiments of the inventions will be apparent to those skilled in the art from consideration of the specification and practice of the inventions disclosed herein. It is intended that the specification and examples be considered as exemplary only, with a true scope and spirit of the inventions being indicated by the following claims.