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DNFSB spots possible bottleneck in Hanford’s waste vitrification
Workers change out spent 27,000-pound TSCR filter columns and place them on a nearby storage pad during a planned outage in 2023. (Photo: DOE)
While the Department of Energy recently celebrated the beginning of hot commissioning of the Hanford Site’s Waste Treatment and Immobilization Plant (WTP), which has begun immobilizing the site’s radioactive tank waste in glass through vitrification, the Defense Nuclear Facilities Safety Board has reported a possible bottleneck in waste processing. According to the DNFSB, unless current systems run efficiently, the issue could result in the interruption of operations at the WTP’s Low-Activity Waste Facility, where waste vitrification takes place.
During operations, the LAW Facility will process an average of 5,300 gallons of tank waste per day, according to Bechtel, the contractor leading design, construction, and commissioning of the WTP. That waste is piped to the facility after being treated by Hanford’s Tanks Side Cesium Removal (TSCR) system, which filters undissolved solid material and removes cesium from liquid waste.
According to a November 7 activity report by the DNFSB, the TSCR system may not be able to produce waste feed fast enough to keep up with the LAW Facility’s vitrification rate.
James P. Adams, Victor T. Berta
Nuclear Technology | Volume 58 | Number 2 | August 1982 | Pages 294-309
Technical Paper | Material | doi.org/10.13182/NT82-A32938
Articles are hosted by Taylor and Francis Online.
Self-powered neutron detectors (SPNDs) with cobalt emitters exhibited sensitivity to water density variations in the loss-of-fluid test large break transient simulations. Definite correlations were determined for both depressurization (decreasing water inventory) and core reflood (increasing water inventory) phases of the transients. The SPNDs were positioned in a radial array at the elevation corresponding to the maximum power in the core. The pre-experiment steady-state power density at the detector locations varied from a maximum of 39.3 kW/m (12.0 kW/ft) to a minimum value of 17.4 kW/m (5.3 kW/ft), inclusive of all locations and transient simulations. All of the SPND data exhibited good correlation to water density variations over this range of initial power densities. Water density fluctuations were measured by the SPNDs throughout these transients, and the fluctuations associated with the early corewide rewet and the gravity reflood flow oscillations are addressed in detail. Analytical investigation of the response of these detectors to water density variations long after reactor shutdown indicates that these detectors will remain sufficiently sensitive to have application in reactor vessel liquid level measurement in small break pressurized water reactor transients.