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2026 ANS Annual Conference
May 31–June 3, 2026
Denver, CO|Sheraton Denver
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NRC commissioners talk reforms, roles at Day 1 of RIC 2026
Even a last-minute cancelation from Department of Energy Secretary Chris Wright could not derail the optimism permeating day 1 of the Nuclear Regulatory Commission’s annual Regulatory Information Conference (RIC).
The optimistic theme came up several times during the morning plenary sessions that highlighted Tuesday’s agenda. The NRC commissioners who spoke said the optimism was a result of the “nuclear renaissance” they are encountering that feels different from past nuclear-related revivals that didn’t materialize.
Miguel Morales Gutierrez, Stefano Caruso, Nikitas Diomidis (Nagra)
Proceedings | 16th International High-Level Radioactive Waste Management Conference (IHLRWM 2017) | Charlotte, NC, April 9-13, 2017 | Pages 498-505
According to the Swiss disposal concept, the safety of a deep geological repository for spent nuclear fuel (SNF) is based on a multi-barrier system. The disposal canister is an important component of the engineered barrier concept, providing containment of the SNF for at least 10,000 years. This study evaluates the criticality safety and shielding of candidate disposal canister concepts, focusing on the fulfillment of the sub-criticality criterion and on limiting radiolysis processes at the outer surface of the canister which can enhance corrosion mechanisms.
The effective neutron multiplication factor (k-eff) and the surface dose rates are calculated for three different canister designs and material combinations for boiling water reactor (BWR) canisters, containing 12 spent fuel assemblies (SFA), and pressurized water reactor (PWR) canisters, with 4 SFAs. For each configuration, individual criticality and shielding calculations are carried out using the SCALE6.2 package (KENO-VI for criticality; MAVRIC for shielding). The results show that k-eff falls below the defined upper safety limit (USL) of 0.95 for all BWR configurations, while staying above USL for the PWR ones. For a final burnup of 55MWd/kgHM and 30y cooling time, the combined photon-neutron surface dose rate is well below the defined limit of 1Gy/h in all cases.