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 />
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