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 />
(~15 s -1 ) than at 25 Hz, the<br />
de<strong>for</strong>mation leads to work<br />
hardening and reduces the<br />
tendency <strong>for</strong> recovery process.<br />
This situation makes the<br />
material less ductile and leads<br />
to fracturing of the material.<br />
The harder material at the<br />
surface results in surface cracks<br />
and material removal. In view<br />
of the above, the wear is high<br />
at 75 Hz. At 125 Hz, the higher<br />
de<strong>for</strong>mation speed (~25 s -1 )<br />
results in higher temperature at<br />
the tip of the pin. The<br />
calculated rise in the<br />
temperature is above<br />
1223 K. This increase in<br />
temperature induces the<br />
oxidation of the surface. The<br />
oxide layer thus <strong>for</strong>med on the<br />
sliding surfaces <strong>for</strong>ms a glazing<br />
layer. Moreover, the oxide layer<br />
is stronger than that of the base<br />
material. Because of the<br />
presence of glazed layer the<br />
wear rate is low at 125Hz. Fig.<br />
3(a-b) reveals the presence of<br />
oxide particles in the<br />
microstructure of the wear scar.<br />
The Topography of the scar was<br />
examined using 3D surface<br />
profilometer and it is presented<br />
in Fig. 3(c). Fig. 3(c) shows that<br />
the scar was covered with a<br />
layer of material of about 2 mm<br />
thickness. This layer could be<br />
oxide layer. Tests were also<br />
per<strong>for</strong>med at a load of 100 N<br />
at 125 Hz and at 823 K to<br />
confirm the influence of heat<br />
generated during fretting on the<br />
<strong>for</strong>mation of oxide layers.<br />
The above observations<br />
reveal that the wear rate is<br />
higher at 125 Hz. In the steam<br />
generator of PFBR, the level of<br />
oxygen is 2 ppm hence, it is<br />
essential to carry out insotdium<br />
tests at 125 Hz.<br />
III.C.8. Effect of Flowing Sodium on<br />
Corrosion and Tensile Properties of AISI Type 316LN<br />
Stainless Steel at 823 K<br />
Austenitic stainless steels (SS)<br />
of different grades are used as<br />
structural materials in primary<br />
circuit, IHX and piping in<br />
secondary loop of fast breeder<br />
reactors owing to their good<br />
compatibility with sodium in<br />
addition to their desirable<br />
properties of adequate high<br />
temperature mechanical<br />
properties and resistance to<br />
neutron irradiation. Sodium is<br />
used as coolant in liquid metal<br />
fast breeder reactors due to its<br />
multifaceted properties of high<br />
thermal conductivity, low<br />
vapour pressure, high boiling<br />
point, large heat capacity and<br />
low cost.<br />
Long term exposure of<br />
austenitic SS to high<br />
temperature sodium leads to<br />
mass transfer and corrosion.<br />
This corrosion is predominantly<br />
governed by the impurities<br />
present in the sodium,<br />
especially carbon and oxygen.<br />
Presence of oxygen in sodium<br />
significantly influences the<br />
corrosion processes because<br />
leaching is usually preceded by<br />
the <strong>for</strong>mation of ternary<br />
compounds of the steel<br />
constituents with oxygen and<br />
sodium. The most commonly<br />
encountered corrosion product<br />
in sodium containing less than<br />
10 ppm oxygen is NaCrO 2 . The<br />
transfer of elements from<br />
structural materials by liquid<br />
sodium is reported to influence<br />
Fig.1 Microstructure showing<br />
316modified layer<br />
R&D FOR FBRs 55