nuclear fuel pellets
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2021 ◽  
pp. 153444
Author(s):  
Murali Krishna Tummalapalli ◽  
Jerzy A. Szpunar ◽  
Anil Prasad ◽  
L.inu Malakkal ◽  
Lukas Bichler

2021 ◽  
pp. 153004
Author(s):  
Ju-Yuan Yeh ◽  
Benjamin W. Spencer ◽  
Sobhan Patnaik ◽  
Travis W. Knight ◽  
Mary Lou Dunzik-Gougar

2020 ◽  
Vol 539 ◽  
pp. 152295
Author(s):  
Heung Soo Lee ◽  
Dong-Joo Kim ◽  
Dong-Seok Kim ◽  
Dong Rip Kim

Author(s):  
Zehua Ma ◽  
Koroush Shirvan ◽  
Wei Li ◽  
Yingwei Wu

Abstract In a light-water reactor, during normal operating condition, the UO2 nuclear fuel pellets undergo fragmentation primarily due to presence of thermal stresses, fission gas development and pellet-clad mechanical interaction. Under Loss of Coolant Accident (LOCA) conditions, a portion of fuel fragments can freely move downwards to the ballooning region due to the significant cladding deformation. The fuel relocation can localize the heat load and in turn accelerate the cladding balloon and burst process. Cladding burst is of great concern because of the potential for fuel dispersal into coolant and clad structural stability. In our work, we built up a finite element model considering cladding balloon, fuel relocation and its resultant thermal feedback during LOCA condition with ABAQUS. The clad balloon model includes phase transformation, swelling, thermal and irradiation creep, irradiation hardening and annealing and other important thermal-mechanical properties. The mass of relocation model was verified against the analytical cases of single balloon and twin balloons. The cladding balloon model combined with fuel thermal conductivity degradation was verified against fuel performance code, FRAPTRAN. Finally, with the evolution of pellet-cladding gap, the fuel mass relocation was calculated and compared against the IFA-650.4 transient test from the Halden reactor.


2020 ◽  
Vol 357 ◽  
pp. 110383
Author(s):  
Thibault Vidal ◽  
Laurent Gallais ◽  
Romain Burla ◽  
Frederic Martin ◽  
Hélène Capdevila ◽  
...  

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