IGCAR : Annual Report - Indira Gandhi Centre for Atomic Research
IGCAR : Annual Report - Indira Gandhi Centre for Atomic Research
IGCAR : Annual Report - Indira Gandhi Centre for Atomic Research
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IGC<br />
<strong>Annual</strong> <strong>Report</strong> 2007<br />
IV.C.6. Temperature Evolution in Spent Fuel Subassembly<br />
during Handling in Fuel Transfer Cell<br />
Spent fuel subassembly (FSA)<br />
is removed from the sodium<br />
filled transfer pot at the<br />
location of Ex-Vessel Transfer<br />
Post (EVTP) <strong>for</strong> handling in Fuel<br />
Transfer Cell (FTC) and<br />
subsequent storage in water<br />
pool storage bay. To prevent<br />
possible release of radioactivity<br />
due to failure of FSA clad, the<br />
temperature of clad should not<br />
exceed its permissible limit of<br />
923 K. To achieve this, the FSA<br />
is <strong>for</strong>ce cooled from the top of<br />
the FSA by supplying nitrogen<br />
at 323 K filled in FTC itself in<br />
re-circulation mode (Fig. 1). In<br />
the event of loss of <strong>for</strong>ced<br />
cooling, the temperatures of<br />
clad and hexcan increase, till<br />
the heat loss under natural<br />
convection and radiation<br />
equals the decay power. It is<br />
essential to determine the final<br />
steady state values of these<br />
temperatures, to assess whether<br />
natural cooling adequate. Also,<br />
knowledge of transient<br />
temperature evolution in the<br />
FSA is essential to determine<br />
the time available <strong>for</strong> the<br />
operator to take safety action.<br />
These have been evaluated by<br />
detailed<br />
conjugate<br />
computational fluid dynamics<br />
studies.<br />
In the absence of <strong>for</strong>ced<br />
cooling, the mode of heat<br />
transfer within the bundle (i.e)<br />
between the pins is only<br />
conduction and radiation as<br />
natural convection of nitrogen<br />
through the compact fuel<br />
bundle is negligible. Heat<br />
transfer from hexcan to FTC<br />
ambient (nitrogen) is by natural<br />
convection and radiation. A 30<br />
degree sector of FSA with the<br />
active fuel pin region of 1 m<br />
height has been considered in<br />
the analysis. For a single pin,<br />
the temperature difference<br />
Fig.1 Spent fuel subassembly <strong>for</strong>ce cooled by nitrogen from top<br />
112 FUEL CYCLE