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Fuel loading process begins at Palisades
The Palisades nuclear power plant has drawn closer to restart, as plant staff began the process of loading fuel into the reactor vessel on Sunday morning.
The commencement of fuel loading places the Covert, Mich., facility in Mode 6—or the refueling stage—under the plant’s technical specifications, plant owner and operator Holtec International said in a news release. The Palisades reactor core consists of 204 fuel assemblies that include new fuel and partially used fuel from the plant’s most recent operating cycles. According to Holtec, the fuel loading is being conducted in accordance with plant procedures and technical specifications.
Isdandy Rezki Febrianto, Anhar Riza Antariksawan, Syarip Syarip, Kevin Rezon
Nuclear Science and Engineering | Volume 200 | Number 5 | May 2026 | Pages 1094-1101
Research Article | doi.org/10.1080/00295639.2025.2504739
Articles are hosted by Taylor and Francis Online.
An analysis of a target system on a small-scale electron accelerator-driven system (e-ADS) for experimental purposes has been conducted. The methodology employed includes particle transport simulations using the Particle and Heavy Ion Transport System (PHITS) code and Response Surface Methodology (RSM) analysis performed with Minitab software. The independent variables reviewed are the energy and radius of the electron beam, as well as the thickness and radius of both the pitcher and the catcher. The dependent variable observed is the neutron yield. Tungsten is used as the pitcher material, while the catcher material is varied among iridium, platinum, tungsten, uranium, thorium, and lead. The RSM analysis indicates that the most optimal target system configuration is tungsten-tungsten, with a pitcher thickness and radius of 1.7 and 3.4 cm, respectively, and a catcher thickness and radius of 1.0 and 2.7 cm, respectively. To achieve the desired neutron output, the required beam parameters are a radius of 0.4071 cm, a current of 1 µA, and an electron energy of 100 MeV, respectively. This configuration produces a neutron yield of 5.764 × 1011 n/s, with a simulation deviation of 0.85%, which is considered acceptable for experimental purposes.