Stability and open circuit breakdown of the passive oxide film on titanium

1988 ◽  
Vol 33 (8) ◽  
pp. 1143-1149 ◽  
Author(s):  
D.J. Blackwood ◽  
L.M. Peter ◽  
D.E. Williams
2014 ◽  
Vol 936 ◽  
pp. 1120-1124 ◽  
Author(s):  
Ahsan Ejaz ◽  
Zhan Peng Lu ◽  
Jun Jie Chen ◽  
Xiao Feng Xia ◽  
Qian Xiao ◽  
...  

The effects of charged hydrogen in iron on surface properties of iron in pure water and sodium sulfate solutions of various concentrations were investigsted by open circuit potential monitoring, surface morphology observations, Raman spectroscopy and XRD measurements. Hydrogen in iron shifed the open circuit potential in the negative directions. Hydrogen could change the types of oxide film on iron. Effects of hydrogen on corrosion of iron was More significant in pure water and dilute sodium solutions than those in concentrated solutions.


1997 ◽  
Vol 79 (21) ◽  
pp. 4282-4285 ◽  
Author(s):  
Michael Toney ◽  
Alison Davenport ◽  
Lucy Oblonsky ◽  
Mary Ryan ◽  
Carissima Vitus

1986 ◽  
Vol 31 (10) ◽  
pp. 1299-1303 ◽  
Author(s):  
R. Goetz ◽  
B. MacDougall ◽  
M.J. Graham

Materials ◽  
2019 ◽  
Vol 12 (21) ◽  
pp. 3466 ◽  
Author(s):  
Okazaki

The oxide film resistance (RP) and capacitance (CCPE) diagrams of implantable metals (commercially pure Ti, four types of Ti alloys, Co–28Cr–6Mo alloy, and stainless steel) were investigated by electrochemical impedance spectroscopy (EIS). The thin oxide film formed on each implantable metal surface was observed in situ by field-emission transmission electron microscopy (FE-TEM). The Ti–15Zr–4Nb–1Ta and Ti–15Zr–4Nb–4Ta alloys had higher oxygen concentrations in the oxide films than the Ti–6Al–4V alloy. The thickness (d) of the TiO2 oxide films increased from approximately 3.5 to 7 nm with increasing anodic polarization potential from the open-circuit potential to a maximum of 0.5 V vs. a saturated calomel electrode (SCE) in 0.9% NaCl and Eagle’s minimum essential medium. RP for the Ti–15Zr–4Nb–1Ta and Ti–15Zr–4Nb–4Ta alloys was proportional to d obtained by FE-TEM. CCPE was proportional to 1/d. RP tended to decrease with increasing CCPE. RP was large (maximum: 13 MΩ·cm2) and CCPE was small (minimum: 12 μF·cm−2·sn−1, n = 0.94) for the Ti–15Zr–4Nb–(0 to 4)Ta alloys. The relative dielectric constant (εr) and resistivity (kOX) of the oxide films formed on these alloys were 136 and 2.4 × 106–1.8 × 107 (MΩ·cm), respectively. The Ta-free Ti–15Zr–4Nb alloy is expected to be employed as an implantable material for long-term use.


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