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At least 19 records

Some Thermodynamic Features of Uranium–Plutonium Nitride Fuel in the Course of Burnup

Calculation studies on the effect of carbon and oxygen impurities on the chemical and phase compositions of nitride uranium–plutonium fuel in the course of burnup are performed using the IVTANTHERMO code. It is shown that the number of moles of UN decreases with increasing burnup level, whereas UN{sub 1.466}, UN{sub 1.54}, and UN{sub 1.73} exhibit a considerable increase. The presence of oxygen and carbon impurities causes an increase in the content of the UN{sub 1.466}, UN{sub 1.54} and UN{sub 1.73} phases in the initial fuel by several orders of magnitude, in particular, at a relatively low temperature. At the same time, the presence of impurities abruptly reduces the content of free uranium in unburned fuel. Plutonium in the considered system is contained in form of Pu, PuC, PuC{sub 2}, Pu{sub 2}C{sub 3}, and PuN. Plutonium carbides, as well as uranium carbides, are formed in small amounts. Most of the plutonium remains in the form of nitride PuN, whereas unbound Pu is present only in the areas with a low burnup level and high temperatures.

11 NUCLEAR FUEL CYCLE AND FUEL MATERIALS↗

Micro Ion Source Program NA22 Plutonium Detection Portfolio Final Report

The purpose of the micro ion source program was to enhance the performance of thermal ionization mass spectrometry (TIMS) for various actinides and fission products. The proposal hypothesized that when ions are created at the ion optic center of the mass spectrometer, ion transmission is significantly increased and the resulting ion beam is more sharply focused. Computer modeling demonstrated this logic. In order to prove this hypothesis it was first necessary to understand the chemistry and physics governing the particular ion production process that concentrates the emission of ions into a small area. This has been achieved for uranium and technetium, as was shown in the original proposal and the improvement of both the beam transmission and sharpness of focus were proven. Significantly improved analytical methods have been developed for these two elements based upon this research. The iodine portion of the proposal turned out to be impractical due to volatility of iodine and its compounds. We knew this was a possibility prior to research and we proceeded anyway but did not succeed. Plutonium is a potential option, but is not quite up to the performance level of resin beads. Now, we more clearly understand the chemical and physical issues for plutonium, but have not yet translated this knowledge into improved analytical processes. The problems are that plutonium is considerably more difficult to convert to the required intermediate species, plutonium carbide, and the chemical method we developed that works with uranium functions only moderately well with plutonium. We are of the opinion that, with this knowledge, similar progress can be made with plutonium.

07 ISOTOPE AND RADIATION SOURCES↗

Investigation of Fission Product Interaction with the SiC Containment Layer of High Turnup TRISO Fuel Particles

Tri-structural Isotropic (TRISO) encapsulated fuel particles are used in high-temperature gas-cooled nuclear reactors. Fuel performance is limited by the propensity of metallic fission products to be released under high temperature testing to simulate hypothesized accident scenarios. The current particle design consists of a 350 μm or 425 μm UO{sub 2} or UCO fuel kernel surrounded by a 100μm porous carbon buffer layer, a 40μm inner pyrolytic carbon (IPyC) layer, a 35μm high-density silicon carbide (SiC) layer, and a 40μm outer pyrolytic carbon (OPyC) layer. Of interest is the fission product interaction with the SiC layer, which provides the most structural support and is the main barrier to the diffusion of fission products. Previous laboratory examination studies have indicated the release of Ag through seemingly intact particles and the localized corrosion of the SiC due to Pd. Although a number of studies have been conducted, the specifics of both the Ag and Pd reaction mechanisms, in addition to U and Pu, through SiC are currently not well understood. This work aims to understand the pathways and kinetics of these interactions under normal operation as well as accident conditions. In order to improve our understanding of this, we have the unique opportunity to examine irradiated TRISO particles to study post-irradiation effects on these materials. Experimental data is necessary to constrain the current models used to predict the behavior of fission products in the SiC layer of TRISO fuels. This work aims to understand the interaction of fission products with the SiC containment layer in TRISO particles. We have systematically examined three SiC shells from irradiated TRISO particles using XAFS, TEM, and EDS. Results indicate the formation of palladium silicides, and uranium and plutonium carbides. Additionally, silver is seen to be metallic. Preliminary microscopy results indicate fission products throughout the SiC layer of the TRISO particles, and microstructural changes have been observed between the as-irradiated and safety tested particles. These results have provided key information on the fission product transport behavior through irradiated SiC at varying temperatures. Knowledge of these reaction pathways will allow for better simulation of the long-term behavior of TRISO fuels. They may also suggest ways to modify the SiC layer to improve fuel performance and mitigate fission product release, which is critical for safety strategies required to commercialize these nuclear fuel technologies. (authors)

11 NUCLEAR FUEL CYCLE AND FUEL MATERIALS↗

Materials Data on La2C3 by Materials Project

La2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. La3+ is bonded in a 9-coordinate geometry to nine equivalent C2- atoms. There are a spread of La–C bond distances ranging from 2.70–3.00 Å. C2- is bonded in a 5-coordinate geometry to six equivalent La3+ and one C2- atom. The C–C bond length is 1.33 Å.

36 MATERIALS SCIENCE↗

Materials Data on Lu2C3 by Materials Project

Lu2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Lu3+ is bonded in a 6-coordinate geometry to nine equivalent C2- atoms. There are a spread of Lu–C bond distances ranging from 2.44–2.75 Å. C2- is bonded to six equivalent Lu3+ and one C2- atom to form a mixture of distorted edge, corner, and face-sharing CLu6C trigonal bipyramids. The C–C bond length is 1.35 Å.

36 MATERIALS SCIENCE↗

Materials Data on Sc2C3 by Materials Project

Sc2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Sc2+ is bonded in a 6-coordinate geometry to nine equivalent C+1.33- atoms. There are a spread of Sc–C bond distances ranging from 2.34–2.65 Å. C+1.33- is bonded to six equivalent Sc2+ and one C+1.33- atom to form a mixture of distorted corner, edge, and face-sharing CSc6C trigonal bipyramids. The C–C bond length is 1.34 Å.

36 MATERIALS SCIENCE↗

Materials Data on Y2C3 by Materials Project

Y2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Y3+ is bonded in a 9-coordinate geometry to nine equivalent C2- atoms. There are a spread of Y–C bond distances ranging from 2.52–2.83 Å. C2- is bonded to six equivalent Y3+ and one C2- atom to form a mixture of distorted edge, face, and corner-sharing CY6C trigonal bipyramids. The C–C bond length is 1.34 Å.

36 MATERIALS SCIENCE↗

Materials Data on Nd2C3 by Materials Project

Nd2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Nd3+ is bonded in a 9-coordinate geometry to nine equivalent C2- atoms. There are a spread of Nd–C bond distances ranging from 2.64–2.94 Å. C2- is bonded to six equivalent Nd3+ and one C2- atom to form a mixture of distorted edge, corner, and face-sharing CNd6C trigonal bipyramids. The C–C bond length is 1.33 Å.

36 MATERIALS SCIENCE↗

Materials Data on Pu2C3 by Materials Project

Pu2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Pu3+ is bonded in a 6-coordinate geometry to nine equivalent C2- atoms. There are a spread of Pu–C bond distances ranging from 2.47–2.80 Å. C2- is bonded to six equivalent Pu3+ and one C2- atom to form a mixture of distorted edge, corner, and face-sharing CPu6C trigonal bipyramids. The C–C bond length is 1.39 Å.

36 MATERIALS SCIENCE↗

Materials Data on Ce2C3 by Materials Project

Ce2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Ce3+ is bonded in a 6-coordinate geometry to nine equivalent C2- atoms. There are a spread of Ce–C bond distances ranging from 2.55–2.87 Å. C2- is bonded to six equivalent Ce3+ and one C2- atom to form a mixture of distorted face, edge, and corner-sharing CCe6C trigonal bipyramids. The C–C bond length is 1.37 Å.

36 MATERIALS SCIENCE↗

Materials Data on Dy2C3 by Materials Project

Dy2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Dy3+ is bonded in a 6-coordinate geometry to nine equivalent C2- atoms. There are a spread of Dy–C bond distances ranging from 2.51–2.82 Å. C2- is bonded to six equivalent Dy3+ and one C2- atom to form a mixture of distorted face, edge, and corner-sharing CDy6C trigonal bipyramids. The C–C bond length is 1.34 Å.

36 MATERIALS SCIENCE↗

Materials Data on Ho2C3 by Materials Project

Ho2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Ho3+ is bonded in a 6-coordinate geometry to nine equivalent C2- atoms. There are a spread of Ho–C bond distances ranging from 2.50–2.80 Å. C2- is bonded to six equivalent Ho3+ and one C2- atom to form a mixture of distorted corner, edge, and face-sharing CHo6C trigonal bipyramids. The C–C bond length is 1.34 Å.

36 MATERIALS SCIENCE↗

Materials Data on Rb2O3 by Materials Project

Rb2O3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Rb is bonded in a 6-coordinate geometry to nine equivalent O atoms. There are a spread of Rb–O bond distances ranging from 2.85–3.18 Å. O is bonded to six equivalent Rb and one O atom to form a mixture of distorted corner, edge, and face-sharing ORb6O pentagonal bipyramids. The O–O bond length is 1.41 Å.

36 MATERIALS SCIENCE↗

Materials Data on U2C3 by Materials Project

U2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. U6+ is bonded in a 6-coordinate geometry to six equivalent C4- atoms. There are three shorter (2.44 Å) and three longer (2.53 Å) U–C bond lengths. C4- is bonded to four equivalent U6+ and one C4- atom to form a mixture of distorted edge and corner-sharing CU4C trigonal bipyramids. The C–C bond length is 1.44 Å.

36 MATERIALS SCIENCE↗

Materials Data on Sm2C3 by Materials Project

Sm2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Sm3+ is bonded in a 9-coordinate geometry to nine equivalent C2- atoms. There are a spread of Sm–C bond distances ranging from 2.59–2.90 Å. C2- is bonded to six equivalent Sm3+ and one C2- atom to form a mixture of distorted edge, face, and corner-sharing CSm6C trigonal bipyramids. The C–C bond length is 1.33 Å.

36 MATERIALS SCIENCE↗

Materials Data on Pr2C3 by Materials Project

Pr2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Pr3+ is bonded in a 9-coordinate geometry to nine equivalent C2- atoms. There are a spread of Pr–C bond distances ranging from 2.66–2.96 Å. C2- is bonded in a 5-coordinate geometry to six equivalent Pr3+ and one C2- atom. The C–C bond length is 1.33 Å.

36 MATERIALS SCIENCE↗

Materials Data on Tb2C3 by Materials Project

Tb2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Tb3+ is bonded in a 9-coordinate geometry to nine equivalent C2- atoms. There are a spread of Tb–C bond distances ranging from 2.53–2.84 Å. C2- is bonded to six equivalent Tb3+ and one C2- atom to form a mixture of distorted corner, edge, and face-sharing CTb6C trigonal bipyramids. The C–C bond length is 1.34 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er2C3 by Materials Project

Er2C3 is Plutonium carbide structured and crystallizes in the cubic I-43d space group. The structure is three-dimensional. Er3+ is bonded in a 6-coordinate geometry to nine equivalent C2- atoms. There are a spread of Er–C bond distances ranging from 2.48–2.79 Å. C2- is bonded to six equivalent Er3+ and one C2- atom to form a mixture of distorted face, edge, and corner-sharing CEr6C trigonal bipyramids. The C–C bond length is 1.34 Å.

36 MATERIALS SCIENCE↗