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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.
A. Bengoechea, G. Noguere, D. Bernard, P. Tamagno
Nuclear Science and Engineering | Volume 200 | Number 1 | March 2026 | Pages S234-S244
Research Article | doi.org/10.1080/00295639.2024.2439676
Articles are hosted by Taylor and Francis Online.
The double-differential scattering cross section for a nucleus with pronounced resonances can be calculated using the stochastic method called Doppler Broadening Rejection Correction (DBRC). Its analytical formulation was developed by Rothenstein and Dagan. Both methodologies are based on the Free Gas Model (FGM), so they exclude chemical binding effects. The numerical instability of including chemical bounds can be balanced by the uncoupled phonon approximation (UPA). However, Courcelle showed that the UPA does not asymptotically resume the FGM and proposed an alternative model for correcting the asymptotic form. Preliminary tests on the Courcelle model showed inconsistent results in differential cross sections compared with the DBRC option of Monte Carlo codes in the framework of the FGM. In this work, a corrected version of Courcelle’s model is presented and applied in the FGM to 238U cross sections. The double-differential scattering cross sections calculated at 300 and 1474 K are in good agreement with those provided by the DBRC. The corrected model is consistent with angle-integrated scattering cross sections calculated with NJOY. The introduction of the effective temperature via the Short Collision Time approximation demonstrates the need to use a more complex model to account for crystalline effects.