ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
Explore the many uses for nuclear science and its impact on energy, the environment, healthcare, food, and more.
Explore membership for yourself or for your organization.
Conference Spotlight
2026 Nuclear Energy Conference & Expo (NECX)
August 24–27, 2026
Dallas, TX|Hilton Anatole
Latest Magazine Issues
Jun 2026
Jan 2026
2026
Latest Journal Issues
Nuclear Science and Engineering
August 2026
Nuclear Technology
July 2026
Fusion Science and Technology
Latest News
Launching into tomorrow: NRIC guides new era of research and deployment
In June 2025, the Department of Energy announced the Reactor Pilot Program, an authorization pathway that allowed reactor developers to partner with the DOE to get first-of-a-kind (FOAK) reactors built and tested. Soon after, the DOE rolled out a complementary Fuel Line Pilot Program, which aimed to fast-track fuel projects. In all, 20 projects were accepted into the new programs.
H. Zimmermann
Nuclear Technology | Volume 28 | Number 1 | January 1976 | Pages 127-133
Technical Paper | Fuels for Pulsed Reactor / Fuel | doi.org/10.13182/NT76-A31546
Articles are hosted by Taylor and Francis Online.
The fission gas behavior in oxide fuel elements irradiated within the irradiation program of the Fast Breeder Project was determined. The amount of fission gas was measured in three steps as released fission gas, fission gas retained in bubbles and pores, and fission gas retained in the fuel matrix. This was done by the puncturing of the fuel rods, by the grinding of the fuel, and by the chemical solution of the powdered fuel, respectively. Under the conditions prevailing in fast breeder reactors, the fractional fission gas release is ∼90% or more after medium and high burnups. The release rate is not constant, but there are periods with particularly high release rates (breakaway release). The retained fission gas reaches concentrations of ∼1.5 × 10−2 gas atoms per uranium and plutonium atoms in fuel regions with temperatures below 1100°C. The concentration decreases with increasing temperatures. At temperatures above 1500°C the concentration of the retained gas is ∼2 × 10−4 gas atoms per initial metal atom. Up to five times more fission gas is retained in bubbles and pores than in the matrix. There is a relation between plastic deformation of the cladding by mechanical interaction with the fuel and the concentration of fission gas in bubbles.