On the pitting corrosion resistance of nitrogen alloyed cold worked austenitic stainless steels

Kamachi Mudali, U. ; Shankar, P. ; Ningshen, S. ; Dayal, R. K. ; Khatak, H. S. ; Baldev Raj, (2002) On the pitting corrosion resistance of nitrogen alloyed cold worked austenitic stainless steels Corrosion Science, 44 (10). pp. 2183-2198. ISSN 0010-938X

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Official URL: http://linkinghub.elsevier.com/retrieve/pii/S00109...

Related URL: http://dx.doi.org/10.1016/S0010-938X(02)00035-5

Abstract

Pitting corrosion studies were carried out on cold worked (5%, 10%, 15%, 20%, 30% and 40%) nitrogen-bearing (0.05%, 0.1% and 0.22% N) type 316L austenitic stainless steels in neutral chloride medium. Potentiodynamic anodic polarisation study revealed that cold working up to 20% enhanced the pitting resistance, and thereafter a sudden decrease in pitting resistance was noticed at 30% and 40% cold working. Increase in nitrogen content was beneficial up to 20% cold work in improving the pitting corrosion resistance, beyond which it had a detrimental effect at 30% and 40% cold working. The role of nitrogen in influencing the deformation band width and dislocation configuration is explained based on the results of transmission electron microscopy investigations. Scanning electron microscopy observation of the pitted specimens indicated decreasing size and increasing density of pits, along the deformation bands with increasing nitrogen for 40% cold worked specimens. The macrohardness values increased as the cold working increased from 0% to 40%. X-ray diffraction studies revealed the increased peak broadening of austenite peak {0 2 2} with increase in cold working. The relationship between pitting corrosion and deformation structures with respect to nitrogen addition and cold working is discussed.

Item Type:Article
Source:Copyright of this article belongs to Elsevier Science.
Keywords:Stainless Steels; Polarisation; SEM; TEM; XRD; Pitting Corrosion; Effects of Strain
ID Code:40392
Deposited On:24 May 2011 05:03
Last Modified:24 May 2011 05:03

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