Page 72 - Challenges in Corrosion Costs Causes Consequences and Control(2015)
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50                                INTRODUCTION AND FORMS OF CORROSION

              At low ambient temperatures, oxidation occurs at asperity contacts because of
           frictional heating. At higher ambient temperatures, general oxidation of the entire
           surface occurs and affects wear. In the case of steel, the predominant oxide present
           in the debris depends on the sliding conditions. The predominant oxide at low speeds
           and ambient temperatures is   -Fe O , at intermediate conditions it is Fe O , and at
                                      2  3                           3  4
           high speeds and temperatures the oxide is FeO. Oxidation of iron and many metals
           follows a parabolic law with the oxide

                                         h = Ct 1∕2

           film thickness increasing with the square root of time “t,” h is the thickness, and C is
           the parabolic rate constant at elevated temperatures (60).
              As diffusion is thermally activated, the growth rate in oxide film thickness during
           sliding as a function of temperature follows an Arrhenius equation

                                       K = Ae (−Q∕RT)

           where K is the parabolic rate constant for the growth of the oxide film, A is the
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           Arrhenius constant (kg /m s), Q is the parabolic activation energy associated with
           the oxide (KJ/mol), R gas constant, and T the temperature. It has been observed that
           the Arrhenius constant for sliding is several orders of magnitude larger than that for
           static conditions. The oxidation rate during sliding may result from increased diffu-
           sion rates of ions through a growing oxide film, which has high defect density because
           of mechanical perturbations (60).


           1.7.12  Electric-Arc-Induced Wear
           When a high potential is present over a thin air film in a sliding process, a dielectric
           breakdown occurs, resulting in arcing. During arcing, a relatively high power den-
           sity occurs over a very short period. The HAZ is usually shallow (∼50 μm), and the
           heating results in melting and resolidification, corrosion, hardness changes, and other
           phase changes. Arcing might also cause ablation of material and craters. Any sliding
           or oscillation after an arc may either shear or fracture the lips, leading to three-body
           abrasion, corrosion, surface fatigue, and fretting (60, 63).


           1.7.13  Erosion–Corrosion
           All types of corrosive media such as aqueous solutions’ organic media, gases, and
           liquid metals can cause erosion–corrosion. The corrodents can be a bulk fluid, a
           film, droplets, or an adsorbed substance. Hot gases may oxidize a metal at high
           velocity and abrade the protective scale. Slurries probably cause most damage in
           erosion–corrosion (9, 17). All types of equipment such as pipelines (curves, elbows,
           and T squares) floodgates, pumps, centrifugal fans, helixes, wheels of turbine, tubes
           of intersections of heat exchangers, and measuring devices are subject to this form
           of attack. Most metals and alloys are subject to erosion–corrosion, and the resulting
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