CHEM02200704003 Nilamadhab Pandhy - Homi Bhabha National ...
CHEM02200704003 Nilamadhab Pandhy - Homi Bhabha National ...
CHEM02200704003 Nilamadhab Pandhy - Homi Bhabha National ...
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Chapter 3<br />
S = <br />
<br />
(2)<br />
= S n + S e (3)<br />
Where S n and S e are the energy loss due to nuclear and electronic stopping power. From<br />
the stopping power (S) the projected range (R p ) of the ions with initial energy E 0 inside the target<br />
can be estimated using Eq. (4) [57].<br />
<br />
R p = <br />
<br />
<br />
(4)<br />
In the present investigation, to study the effect of sub-surface modification on the corrosion<br />
resistance of 304L SS, nitrogen ion implantation was carried out at 70 keV energy by 150 keV<br />
accelerator at room temperature using 99.999 % high purity nitrogen on 12 mm diameter<br />
specimens of 304L SS. The doses given were in the range of 1×10 15 , 1×10 16 , 1×10 17 and 2.5×10 17<br />
N + /cm 2 , respectively (Eq. 1). The vacuum in the target side during implantation was maintained at<br />
1×10 -5 Pa. The projected range of the ions in 304L SS was calculated using Monte-Carlo<br />
simulation code Transport of Ions in Matters (TRIM) [57]. TRIM is based upon binary ion-atom<br />
collision approximation assuming moving atom as ion and the target atom as atoms for calculating<br />
the range distribution of ions inside the target. The Monte-Carlo simulation as applied in TRIM<br />
has number of advantages over analytic formulation. It allows rigorous treatment of elastic<br />
scattering, explicit consideration of surface and interfaces leading to easy determination of<br />
projected range and distribution of particles.<br />
3.1.2.2 Magnetron sputtering<br />
Magnetron sputtering is a high vacuum coating process for depositing metals, alloys and<br />
ceramic coatings. Developed in 1970’s, magnetron sputtering is finding increasing application in