An XPS study of passive film formation on Fe 30Mn 9Al alloy in sodium sulphate solution

1998 ◽  
Vol 125 (1) ◽  
pp. 11-16 ◽  
Author(s):  
X.M. Zhu ◽  
Y.S. Zhang
1988 ◽  
Vol 28 (6) ◽  
pp. 559-576 ◽  
Author(s):  
E. McCafferty ◽  
M.K. Bernett ◽  
J.S. Murday

2020 ◽  
Vol MA2020-02 (8) ◽  
pp. 1161-1161
Author(s):  
Yusi Xie ◽  
Minglu Liu ◽  
Ashlee Aeillo ◽  
Karl Sieradzki

2019 ◽  
Vol 166 (11) ◽  
pp. C3071-C3080 ◽  
Author(s):  
Cem Örnek ◽  
Marie Långberg ◽  
Jonas Evertsson ◽  
Gary Harlow ◽  
Weronica Linpé ◽  
...  

CORROSION ◽  
1993 ◽  
Vol 49 (11) ◽  
pp. 877-884 ◽  
Author(s):  
D. Li ◽  
X. Mao ◽  
R. Zhu

Abstract Kinetics of passive film formation on the bare surface of scratched stainless steels SS in magnesium chloride (MgCl2) solutions were studied using the rapid scratching technique under potentiostatic conditions. An experimental device was designed to record data at the rate of 20,000 points/s, with the rotating rate of the specimen at 3,000 rpm and a scratch scar length of about 4.6 mm to 4.8 mm. A new phenomenon was observed in that two peaks were seen rather than a continuous decay in the curve of current decay on scratched SS in MgCl2 solutions. Current decayed steeply to approximately passive current within about 2.5 ms to 3 ms after the diamond knife was moved away from the specimen. Current rose again for about 2 ms to 3 ms. This phenomenon was considered to represent the processes of adsorbed layer formation on the bare surface and transformation of the adsorbed layer into a passive film. Results were affected by the recording rate of experimental data, the specimen rotating rate, and the scratch scar length. The kinetics of passive film growth were shown empirically by i(t) = I0exp(−βt) with I0 and β being constants. Passive film growth was controlled by ion conduction in a strong electric field, as defined by i = A exp(BV/x).


1989 ◽  
Vol 66 (8) ◽  
pp. 3942-3945
Author(s):  
D. B. Hagan ◽  
B. W. Sloope ◽  
V. A. Niculescu

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