Thermal Analysis Evaluations Using the Dry Cask Simulator

Author(s):  
S. R. Suffield ◽  
D. J. Richmond ◽  
J. A. Fort

Abstract Different thermal analysis models were developed to simulate the dry cask simulator (DCS). The DCS is an experiment designed to simulate dry storage of a single boiling water reactor fuel assembly under a variety of heat loads and internal pressures. The DCS was set up and tested in both a vertical and horizontal configuration to determine cladding temperatures in vertical and horizontal dry cask storage systems. The models included a detailed STAR-CCM+ model with the fuel assembly geometry explicitly modeled, a porous STAR-CCM+ model with the fuel assembly geometry modeled as a porous media region with calculated effective properties, and a COBRA-SFS model. COBRA-SFS is a thermal-hydraulic code developed for steady-state and transient analysis of multi assembly spent-fuel storage and transportation systems. STAR-CCM+ is a commercial computational fluid dynamics (CFD) code. Both a detailed and porous STAR-CCM+ model were developed to look at the effective thermal conductivity (keff) approach to modeling a fuel assembly. A keff fuel model is typically modeled in CFD thermal analyses due to its significantly lower computational costs. The models were run for a combination of low and high canister pressures (100 kPa and 800 kPa) and low and high internal heat loads (0.5 kW and 5 kW). Results from all three models were compared against experimental data taken from the DCS for the peak cladding temperature (PCT) and inlet air mass flow.

1989 ◽  
Vol 111 (4) ◽  
pp. 647-651 ◽  
Author(s):  
J. Y. Hwang ◽  
L. E. Efferding

A thermal analysis evaluation is presented of a nuclear spent fuel dry storage cask designed by the Westinghouse Nuclear Components Division. The cask is designed to provide passive cooling of 24 Pressurized Water Reactor (PWR) spent fuel assemblies for a storage period of at least 20 years at a nuclear utility site (Independent Spent Fuel Storage Installation). A comparison is presented between analytical predictions and experimental results for a demonstration cask built by Westinghouse and tested under a joint program with the Department of Energy and Virginia Power Company. Demonstration testing with nuclear spent fuel assemblies was performed on a cask configuration designed to store 24 intact spent fuel assemblies or canisters containing fuel consolidated from 48 assemblies.


Author(s):  
Xinyu Wang ◽  
Richard Cable Kurwitz ◽  
Zhijian Zhang

This paper is the optimization of fuel assembly placement in the spent fuel pool according to the categorized rules. Only some specifically reactivity class assemblies could put together as the pattern. The allowable patterns, the number of the fuel assembly for each reactivity class and the number of RCCAs are from the nuclear power plant technique specification. Each assembly in the pool should obey the pattern rules and the user needs the optimal spent fuel pool configuration that could maximize the free space. In this study, the genetic algorithm and greedy algorithm are discussed, and both of two algorithms have the difficulties to the real engineering problem. A new approach that improves the greedy strategy at each step is proposed, make the greedy algorithm is more adapted to the engineering problem. Use the new approach to test Seabrook Unit 1 and Arkansas Unit 2 spent fuel pool at different cases, and show results by the visible figures. The output arrangements by the program shown that the results are satisfied the user requirements.


Author(s):  
Mikal A. McKinnon ◽  
Judith M. Cuta ◽  
Urban P. Jenquin

Abstract As part of a cooperative program, the United States Department of Energy (DOE) has supported analyses to determine the effect of cask loading on the thermal and shielding performance of a cask containing spent nuclear fuel. Two considerations that must be addressed in licensing spent fuel storage casks are peak fuel temperature and cask surface dose rate. Generally, storage systems are approved for uniform loading of the cask with design basis fuel. The storage system design basis typically specifies maximum assembly enrichment, maximum burnup, and minimum cooling times for the design basis fuel. Some casks specify an enrichment/burnup table. These conditions set the maximum decay heat loads and maximum radioactive source terms for the design. Supportive analysis using conservative assumptions is then used to demonstrate that acceptable fuel storage temperatures and cask dose rates are maintained. This study analyzes the effect of non.-uniform load patterns on peak fuel cladding temperatures and cask surface dose rates using previously validated analytical methods. The study was performed using a spent fuel storage cask that was designed to hold 24 spent fuel assemblies with a decay heat load of 24 kW. The cask was assumed to have a forged steel body with an overall length of 5.0 m and a diameter of 2.3 m. The body was assumed to be surrounded by a resin layer for neutron shielding and a steel outer shell. The fuel was selected to have cooling times of 3.5 to 10 years and burnups of 20 to 60 GWd/MTU to bound the expected range of burnup for most of the fuel to be discharged from boiling water and pressurized water reactors from the mid-1970s through 2020. Three radial power distributions were considered in the study: uniform loading, hotter assemblies in the center of the cask, and hotter assemblies near the wall of the cask. Each load pattern resulted in a total decay heat output of 24 kW from the cask. Seventeen different load patterns were selected, and the thermal analysis was repeated for three backfill gases: helium, nitrogen, and vacuum. For a given decay heat load in the cask, loading assemblies with higher decay heat output around the outside of the cask results in lower peak fuel cladding temperatures than loading hotter assemblies in the center of the cask. Several of the load patterns resulted in a peak cladding temperature that was lower than for a uniformly loaded cask. For a helium backfill with an optimum load pattern in the cask (hot assemblies near the basket wall), the peak fuel clad temperature was 17°C lower than a uniformly loaded cask. Using the same assemblies from the optimum load pattern but reversing the load pattern so the hot assemblies are moved to the inside of the cask., increased the peak fuel clad temperatures by 35°C for a helium backfill. This is 18°C greater than for a uniform load pattern. Seven source terms were selected to provide the thermal output used in the thermal analysis. Source term calculations were completed using fuel burnups of 20 to 60 GWd/MTU and enrichments of 2.4 to 4.8%. A constant power density of 32 MW/MTU was used for all irradiation calculations. Cooling times were selected to provide the decay heat values used in the thermal analysis. Photon dose rates are dominated by the cobalt-60 in the bottom-end fittings, top-end fittings, and plenum and are proportional to fuel burnup. For short cooling times, photon dose rates on the side of the cask are somewhat higher due to short-lived fission products. Cask loadings with high decay heat assemblies near the periphery exhibit increased photon dose rates on the side surface and top and bottom surfaces away from the centerline. Near the centerline, on the top and bottom of the cask, the dose rates are reduced substantially. Neutron dose rates increase exponentially with burnup and are nearly independent of cooling time. Cask loadings with high decay heat assemblies impact the neutron dose rates minimally. The peak dose rates (neutron plus photon) for the short-cooled, higher-burnup fuel loaded around the outside of the cask’s basket are generally less than for a uniform loading of longer-cooled, higher-burnup spent fuel.


Author(s):  
Akihisa Iwasaki ◽  
Yoshitsugu Nekomoto ◽  
Hideyuki Morita ◽  
Katsuhiko Taniguchi ◽  
Daisaku Okuno ◽  
...  

The spent fuel storage rack of a nuclear plant stores the spent fuel temporarily before it can be moved to a reprocessing facility. Therefore, the spent fuel storage rack must have a high tolerance against large seismic loads. So, the free standing rack is developed in Japan as other countries. The free standing rack structure incorporates the effect of the friction force on the spent fuel pool floor, and the fluid effect. Under earthquake condition, the free standing rack sliding and rocking motions are induced and the spent fuels rattle in the cells. In this paper, sliding and rocking motions of full-scale rack model having full loading fuel assembly subjected to the seismic excitation are studied. To develop an analysis evaluation method for rack motions, we carried out seismic test of a full-scale rack model using a shaking table, and obtained the fundamental data about the free standing rack.


2018 ◽  
Vol 19 ◽  
pp. 36
Author(s):  
Daniel Vlček

This project deals with the thermal analyses of the wet and dry storages of the spent nuclear fuel. The dry spent fuel storage sub-channel code COBRA-SFS has been used in order to calculate the temperature field. In this code, the new model of residual heat removal was created for the SKODA 1000/19 cask where the spent nuclear fuel TVSA-T type from NPP Temelin will be stored. The object of calculations was to obtain the inside temperatures under maximum loads. After that, the results were compared to the requirements of the local regulatory body. Because of the absence of experimental data, the validation of the created computational models could not be accomplished. However, according to the verification scheme of the COBRA-SFS authors, the verification of the new models was implemented.


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