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 />
Experiment to validate failed<br />
fuel detection system<br />
This experiment was<br />
conducted with a special<br />
subassembly having 19<br />
per<strong>for</strong>ated pins (with a total<br />
exposure area of 112.8 cm 2 ) of<br />
natural uranium loaded<br />
successively at five different<br />
locations. The main objectives<br />
of the experiment were:<br />
To calibrate Delayed<br />
Neutron Detection (DND)<br />
system at different power<br />
levels, primary sodium flows<br />
and sodium inlet<br />
temperatures<br />
To establish the feasibility<br />
of localization of failed SA<br />
using DND system<br />
To check the response of<br />
Clad Rupture Detection<br />
(CRD) in argon system<br />
To validate the failed fuel<br />
localization setup.<br />
The results were satisfactory<br />
and validated the ability of the<br />
DND system not only to detect<br />
any clad breach, but also to<br />
broadly identify the zone of<br />
failure from the contrast ratios<br />
of the east & west DND signals.<br />
Failed fuel localisation system,<br />
intended to determine the age<br />
of the fuel per<strong>for</strong>med well in<br />
detecting the presence of Kr<br />
and Xe in cover gas argon.<br />
Residual life assessment of the<br />
grid plate<br />
Grid plate, which supports<br />
entire core, is one of the<br />
important components that limit<br />
the life of the reactor. The life<br />
limiting factors are residual<br />
ductility and swelling.<br />
Displacement per atom (DPA) is<br />
one of the parameters that is<br />
found to have good correlation<br />
with the radiation damage to<br />
the material. However, DPA<br />
cannot be directly measured.<br />
Fluxes above 0.1 MeV<br />
contribute maximum to the<br />
DPA. The fission reactions rates<br />
in 237 Np have good correlation<br />
with the DPA rate, as the crosssection<br />
threshold is around 400<br />
keV. Hence, Neptunium foils<br />
were used to measure the grid<br />
plate fluence. Standard<br />
irradiation experimental<br />
subassembly with a capsule was<br />
used. The special capsule is<br />
made of SS rod containing the<br />
foils at the guide sleeve and<br />
support plate of the grid plate<br />
and core mid plane. As the<br />
capsule is longer than the<br />
standard irradiation capsules,<br />
flow induced vibration test was<br />
carried out with a dummy<br />
subassembly at FRTG and the<br />
vibration found to be<br />
negligible. The subassembly<br />
was loaded in 4th ring of the<br />
core and the reactor operated<br />
at 15.6 MWt <strong>for</strong> about 14 days.<br />
The experimental carrier along<br />
with the capsule was<br />
discharged and sent to RML hot<br />
cell <strong>for</strong> retrieving the foils from<br />
the capsule and counting of<br />
fission product activities.<br />
Concurrently, test specimens of<br />
SS 316 used in the reactor are<br />
also being irradiated to<br />
simulate the damage. They will<br />
be retrieved at the end of the<br />
14 th campaign after 70 days of<br />
irradiation and measurements<br />
of residual ductility and swelling<br />
carried out. The results of both<br />
these experiments will provide<br />
the basis <strong>for</strong> the residual life<br />
assessment of the grid plate.<br />
Irradiation of PFBR test fuel pin<br />
<strong>for</strong> initial gap closure<br />
The peak Linear Heating Rate<br />
(LHR) <strong>for</strong> PFBR fuel is 450<br />
W/cm. From fabrication<br />
considerations, the fuel<br />
fabricator has asked <strong>for</strong><br />
relaxation of the tolerances on<br />
the pellet diameter. This will<br />
result in higher fuel-clad gap,<br />
and the fresh fuel will hence<br />
have to be operated at lower<br />
LHR till the gap closes by<br />
cracking and restructuring of<br />
the fuel. The duration of<br />
operation at low LHR has<br />
implications on the economics<br />
of power generation. To<br />
determine the time required <strong>for</strong><br />
the gap to close, a single pin of<br />
PFBR test fuel was irradiated in<br />
FBTR <strong>for</strong> 14 days. Mixed Oxide<br />
with 29% PuO 2 and rest UO 2<br />
enriched with about 53.5% U 233<br />
is used as fuel <strong>for</strong> this pin.<br />
2 FAST BREEDER TEST REACTOR