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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

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