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
Jul 2026
Jan 2026
2026
Latest Journal Issues
Nuclear Science and Engineering
August 2026
Nuclear Technology
July 2026
Fusion Science and Technology
Latest News
The deadline arrives: Checking in on the Reactor Pilot Program
On May 23, 2025, President Trump signed Executive Order 14301, “Reforming Nuclear Reactor Testing at the DOE,” which instructed the Department of Energy to create a Reactor Pilot Program (RPP)—a new system in which companies could pursue DOE authorization to build and test their first-of-a-kind nuclear technologies. EO 14301 set an ambitious goal for that program: three reactors achieving criticality by July 4, 2026.
R. A. Karam, K. D. Dance, T. Nakamura, J. E. Marshall
Nuclear Science and Engineering | Volume 40 | Number 3 | June 1970 | Pages 414-423
Technical Paper | doi.org/10.13182/NSE70-A20193
Articles are hosted by Taylor and Francis Online.
An integral transport method was developed and applied to the calculation of the central reactivity worths of various samples measured in a 2700-liter uranium-carbide fast core and in a 4000-liter UO2 fast core. The method was used to obtain corrections to multigroup first-order perturbation calculations, incorporating self-shielding effects inside and outside the sample, as well as scattering, fission, and edge-effect perturbations. Resonance interaction between a 238U sample and the 238U in the core as well as resonance self-shielding in the sample itself were explicitly considered. A similar treatment was used for 235U samples. ENDF/B data were used in all of the analyses. The calculated central worths of 10B and tantalum were in very good agreement with the measured values, indicating that the calculated value of βeff used to convert percent Δk/k to period measurements was reasonably accurate. The calculated worths of 235U were 5 to 10% greater than the measured values. The discrepancy between the calculated and measured values for 238U was 15 to 20%. The discrepancy for graphite in particular and scatterers in general was rather large, indicating that the distribution of the adjoint function is not adequately calculated.