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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 />

Fig.2 Computational mesh of 30 o<br />

sector of FSA<br />

Fig.3 Steady state temperature of<br />

fuel pins and nitrogen (in K) <strong>for</strong><br />

5 kW decay power<br />

between the fuel centre and<br />

clad surface is estimated as ~<br />

1 K only due to very low decay<br />

power of 5 kW. Hence, the fuel,<br />

clad and the gap between them<br />

are lumped into a single<br />

material having equivalent<br />

properties. The finite volume<br />

mesh of the FSA generated<br />

using STAR-CD code is<br />

presented in Fig. 2. The decay<br />

power of the FSA is given as<br />

volumetric heat source in the<br />

fuel pins. Appropriate values of<br />

surface emissivity have been<br />

taken <strong>for</strong> clad and hexcan,<br />

considering the fact that<br />

sodium is coated on the<br />

surfaces.<br />

Predicted steady state<br />

temperatures of the fuel pins,<br />

stagnant nitrogen within the<br />

FSA and hexcan, <strong>for</strong> 5 kW<br />

decay power, are presented in<br />

Fig. 3. As the heat transfer<br />

takes place in the radial<br />

direction and towards the heat<br />

sink which is outside the<br />

hexagonal sheath, the pin<br />

surfaces facing the sheath are<br />

at lower temperature compared<br />

to pins surfaces facing the<br />

centre of the FSA. It is seen that<br />

the temperature of central pin<br />

clad is 1557 K. Since the clad<br />

temperature is exceeding 923<br />

K, <strong>for</strong>ced cooling of the FSA is<br />

essential. Similar maximum<br />

clad temperature is estimated<br />

<strong>for</strong> various values of decay<br />

powers (from 1 to 5 kW). It is<br />

Fig.4 Evolution of central pin clad temperature during loss of cooling<br />

(5 kW decay power)<br />

found that <strong>for</strong> a decay power of<br />

1 kW, the clad temperature is<br />

883 K which is within the limit<br />

of 923 K. For 2 kW decay<br />

power (corresponding to<br />

internal storage <strong>for</strong> 2<br />

campaigns), the clad<br />

temperature is 1118 K. Hence,<br />

FSA with decay power less than<br />

or equal to 1 kW can be<br />

handled in FTC without any<br />

<strong>for</strong>ced cooling. For higher<br />

powers, <strong>for</strong>ced cooling is<br />

essential.<br />

The transient temperature<br />

evolution of spent FSA central<br />

pin clad in FTC is presented in<br />

Fig. 4, <strong>for</strong> the case of 5 kW<br />

decay power. The normal fuel<br />

handling time of spent FSA is<br />

30 - 45 min <strong>for</strong> its travel from<br />

primary sodium pool to EVTP.<br />

When the FSA reaches EVTP<br />

after this time, the clad<br />

temperature is ~773 K. At<br />

EVTP location, the FSA is taken<br />

out of the sodium filled transfer<br />

pot and the clad temperature<br />

again starts to increase when<br />

<strong>for</strong>ced cooling is unavailable<br />

<strong>for</strong> the FSA inside FTC. It takes<br />

15 min <strong>for</strong> the central pin clad<br />

temperature to reach the<br />

limiting value of 923 K. After<br />

this it takes a long time (~4 h)<br />

to reach the steady state<br />

temperature of 1557 K. Hence,<br />

it is established that loss of<br />

cooling can be sustained <strong>for</strong><br />

about 15 min.<br />

FUEL CYCLE 113

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