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 />
was determined by step height<br />
measurements. Figure 1 shows<br />
the void swelling in the two<br />
alloys as a function of the<br />
irradiation temperature. It is<br />
found that the peak swelling<br />
temperatures and the<br />
magnitude of swelling <strong>for</strong> the<br />
two alloys are different.<br />
Whereas the alloy with 0.15%<br />
Ti displayed a swelling of<br />
~15% at the peak swelling<br />
temperature of 923 K, the alloy<br />
with 0.25% Ti has a swelling<br />
maximum of ~ 4% at 823 K.<br />
With similar thermomechanical<br />
treatment effected<br />
on both the alloys the<br />
difference in void swelling<br />
behavior is solely due to the<br />
effect of chemical composition.<br />
In order understand the<br />
drastically different behaviour<br />
of the two alloys with regard to<br />
void swelling, the TiC<br />
precipitate <strong>for</strong>mation in these<br />
two alloys was studied by<br />
positron lifetime measurements.<br />
The un-irradiated alloys were<br />
subjected to isochronal<br />
annealing and the positron life<br />
time was measured after each<br />
annealing. These alloys show<br />
different TiC precipitate<br />
<strong>for</strong>mation behavior (Fig.2). The<br />
observed variation of lifetime τ<br />
displays distinct stages viz., a<br />
monotonic decrease in τ from<br />
the initial cold worked state<br />
upto ~900 K in alloy B and ~<br />
800 K in alloy A. This is<br />
followed by a stage where there<br />
is an increase in lifetime to<br />
saturation, followed by a<br />
decrease in lifetime. The first<br />
stage corresponds to point<br />
defect recovery arising out of<br />
the migration of vacancies to<br />
sinks such as dislocations .The<br />
subsequent stage where there is<br />
an increase in lifetime τ is the<br />
result of positron trapping by<br />
the TiC precipitate which <strong>for</strong>ms<br />
during the heat treatment. The<br />
increase in average lifetime of<br />
positrons in this stage <strong>for</strong> alloy<br />
A in comparison to alloy B is<br />
due to the higher number<br />
density of TiC precipitates in the<br />
<strong>for</strong>mer. The observed lower<br />
void swelling in alloy A can be<br />
attributed to the higher number<br />
density of TiC precipitates .It is<br />
further seen (Fig.2) that there is<br />
a difference in the onset of TiC<br />
precipitation by 100K between<br />
the two alloys. The Shift in the<br />
peaking swelling temperature<br />
can be attributed to the<br />
difference in the onset<br />
temperature <strong>for</strong> TiC<br />
precipitation <strong>for</strong> the two alloys.<br />
Thus, positron lifetime<br />
measurements helps to<br />
rationalize the different swelling<br />
behavior in alloys with different<br />
Ti concentrations.<br />
Fig.1 Temperature dependence of void swelling measured<br />
by surface profilometry <strong>for</strong> the D9alloys with different<br />
titanium concentration<br />
Fig.2 Variation of positron life time with annealing<br />
temperature <strong>for</strong> the cold -worked D9 alloys with<br />
different titanium concentration, alloy A (Ti / C = 6) and<br />
alloy B (Ti /C = 4)<br />
46 R&D FOR FBRs