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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 />

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

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