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Scientific Reports volume 11, Article number: 12602 (2021 ) Cite this article wear plate welding wire
The effect of low oxygen-partial pressured carburizing on relaxation process for 316L stainless steel is reported. Phase, morphology, and amount of compound formation during initial stage of carburizing are investigated using X-ray diffractometry (XRD) and X-ray photoelectron spectroscopy (XPS). The results show formation and development of surface multilayer with nano-grain-carbide (Cr7C3, Fe7C3, and/or Cr3C2) generation in the layer located below outermost protective layer. The relaxation process has been investigated using electrochemical impedance spectroscopy (EIS). Formation of nano-grain carbide(s) during carburizing causes deterioration effect on the electrochemical behavior of steel. However, the steel with large amount of carbide generation (carburized for 30 min) tends to have higher corrosion resistance (indicated by higher values of Rcl and Rct) than the smaller ones (10 and 20 min) due to the effect of phase, grain size, morphology, and amount of compound formation.
Metallic parts used in carbonaceous atmosphere (of carbon monoxide, methane, or other hydrocarbons) are subjected to carburizing. Carburizing is a long-standing corrosion problem in energy conversion and production systems of petrochemical industries including ethylene production1,2,3,4. Carburizing causes reaction between carbon from atmosphere and carbide forming elements in stainless steels such as Cr, Al, Si, and Fe. The carbon uptake and the formation of carbides promote local stresses that affect the mechanical properties of steels1. In operation, the components such as CO2-cooled nuclear reactor, furnace tube, and reformer or pyrolysis tubes4,5,6 are not only subjected to dry corrosion during in-service period but also wet corrosion in out-of-service one. Failure of the parts can lead to a leakage of chemicals which produces pollution problems and approximately 137 quadrillion joules of lost energy2,7. Austenitic stainless steels are extensively used in such carbonaceous atmosphere due to possession of higher carburizing resistance (resulted from lower diffusion coefficient of carbon) than ferritic stainless steels. Regarding the austenitic grades, corrosion and carburizing resistance of 316L stainless steel is superior to the 304 and 316 grades due to addition of Mo and possession of lower carbon content. Moreover, 316L stainless steel has nonmagnetism, good ductility, toughness, and weldability with lower price comparing to Ni-based alloys4,8,9,10. It is well known that the steels are susceptible to wet corrosion in marine environment due to the exposure to Cl–. In such wet or dry corrosion, the protective layer including Cr2O3 plays an important role in the corrosion protection of stainless steels1,11,12,13,14. Carburizing has a detrimental effect on the protective layer by a transport of carbon through Cr2O3 scale which therefore causes the corrosion problems2,15,16. Many research have been reported on only the effect of dry corrosion associated with carburizing, while the important effect of wet corrosion associated with electrochemical process is seemed to be ignored1,2,15,16. Our current study reports on effect of nano-grain carbide formation on electrochemical relaxation process for 316L austenitic stainless steel carburized in low oxygen-partial pressure. Such carbon rich environment corresponds to actual service environment that contains carbon monoxide, methane, or other hydrocarbons1. The effect of carburizing (phase, morphology, and amount of compound formation) on wet corrosion and critical period of service of the steel have been discussed.
Quarter-circle-shaped samples with 19 mm in diameter and 10 mm in height were prepared from (A276) annealed 316L stainless steel rod with chemical composition (wt%) of Fe–16.62Cr–12.00Ni–2.03Mo–0.012C–0.31Si–1.28Mn–0.037P–0.022S. The samples were ground and polished by 2000 grid SiC and 0.3 μm Al2O3. Carburizing was done using a current heating technique as the setup shown in Fig. 1. The sample was ultrasonically cleaned by methanol for 5 min and packed with a pressure of ~ 10.3 kPa in 20 μm-graphite powders placed between two copper electrodes in a glass tube. The chamber was evacuated in order to achieve a condition of low vacuum with absolute pressure of ~ 66 kPa and subsequently fed with 99.99%-purity Ar gas with a flow rate of 50 ml/min. DC current with a power of 300 W was applied to specimens for 10, 20, and 30 min for carburizing which resulted in carburizing temperatures of ~ 350, 550, and 600 °C, respectively. After treatment, the sample was removed and cooled down to ambient temperature in air.
Configuration of current heating system used for carburizing.
Surface morphology of sample was analyzed by X-ray diffractometry (XRD) and X-ray photoelectron spectroscopy (XPS). XRD was performed using Mini Flex II (Rigaku) diffractometer with a Cu Kα X-ray source (1.5406 Å, 30 kV, and 15 mA) at 0.02° step size and 0.3 s step time. The area of 3 × 3 mm on surface of sample was sputtered by Ar+ with 1 keV ion energy for 20 s for removal of some contamination before characterized by XPS. The samples were examined using Kratos Axis ULTRADLD (Kratos) spectrometer equipped with a monochromatic Al Kα X-ray source (1486.6 eV). The base pressure in analysis chamber was approximately 5 × 10–9 torr. The X-ray source was used with the incidence angle of 45° to surface plane. The operation was done at 150 W (15 kV and 10 mA) with a spot size of 700 × 300 µm2 and initial photo energy of 1.4 keV. The binding energy of adventitious C 1 s peak at 285 eV was used for calibration of wavelength shift. The spectra were acquired (at a constant take-off angle of 90°) with the pass energy of 20 eV and analyzed with the energy step of 0.1 eV using VISION II (version 2.2.9) software. Impedance of samples were measured by electrochemical impedance spectroscopy (EIS). EIS measurement was performed using the Autolab-PGSTAT302N potentiostat (Metrohm Autolab B.V.) in aerated 3.5% NaCl solution at ~ 25 °C with a Ag/AgCl reference electrode and a platinum counter electrode incorporated with NOVA (1.11.0) software. The exposed surface area of working electrodes was ~ 0.9–1.0 cm2. Before EIS measurement, the open circuit potential (OCP) of working electrode was monitored for 2000 s or until a stable OCP was achieved. The amplitude of applied sinusoidal potential was 10 mV (r.m.s.) around the OCP and the frequency was controlled to be of between 100 kHz and 0.1 Hz. For each analysis condition, the EIS measurement was performed for at least three times by using a new sample in fresh solution. The closest single result to the average of multiple data was chosen to be the representative of each analysis condition. The electrochemical parameters of steels were determined by fitting the EIS experimental data using NOVA (1.11.0) software.
XRD patterns of the steels are shown in Fig. 2. For untreated steel, three peaks of austenite contributed by (111) (43.472°), (200) (50.673°), and (220) (74.677°) are observed. An additional primary peak of Cr7C3 contributed by (151) (44.599°) is present in the steel treated for 10 min. Peaks contributed by (121) (39.133°) and (003) (26.603°) of Cr3C2 and graphite, respectively, are observed in the steel treated for 20 min (Supplementary material 1). The peak intensity of Cr7C3 is lower than the steel treated for 10 min. The XRD pattern of steel treated for 30 min exhibits contribution of additional Cr7C3 peaks: (150) (39.491°), (112) (42.823°), (222) (50.673°), and (260) (52.551°). Primary peaks of ferrite (contributed by (110) (45.067°)) and Fe7C3 (contributed by (211) (44.855°)) are present close to the primary peak of Cr7C3 which results in peak convolution with asymmetric feature. For low strain material, grain size of the compound can be evaluated using Scherrer's equation:
where Dhkl (Å), K, λ (Å), βhkl (rad), and θ (rad) are average diameter of grain along the [hkl], Scherrer's constant (0.9 for assuming to be a spherical grain), wavelength of X-ray, full-width at a half-maximum of the (hkl) diffraction, and a half of diffraction angle, respectively17,18,19. The values of βhkl and θ for calculation were obtained from the strongest non-overlapping peak of compound in the spectrum (Supplementary material 1). The sizes of nano-grains of Cr7C3 generated in steels treated for 10 (18.34 nm), 20 (10.45 nm), and 30 min (14.2 nm) were evaluated. The grain size of Cr3C2 generated in steel treated for 20 min was 19.75 nm. The thickness of compound layer generated in steels treated for 10 (~ 0.4 μm), 20 (~ 1.5 μm), and 30 min (~ 7.0 μm) were determined from cross-sectional images shown in Supplementary material 2.
XPS results in Fig. 3 show observation of carbides, oxides, hydroxides, carbon-oxide compound, graphite, and free carbon in the steels with binding energies corresponding to the compounds reported in previous research1,12,20,21,22,23,24,25,26,27,28,29,30,31,32,33. The peaks represent to Fe (~ 706.9 eV (Fe 2p))12,20,24,25,26,27 and Cr (~ 573.8 eV (Cr 2p))12,20,22,23,25,26,27 metals were only observed in untreated steel, while Fe2O3 peak (~ 711.2 eV (Fe 2p))20,28 was not observed. For the steel treated for 10 min, the peaks corresponding to FeO (~ 708.7 eV (Fe 2p) and ~ 529.8 eV (O 1s))25,26,28 were observed. For the samples treated for 20 and 30 min, the peaks associated with Cr7C3 (~ 574.7 eV (Cr 2p) and ~ 283.8 eV (C 1s))1,22,33, Cr3C2 (~ 575.8 eV (Cr 2p) and ~ 286.7 eV (C 1s))23, Fe7C3 (~ 707.8 eV (Fe 2p) and ~ 283.8 eV (C 1s))1, and free carbon (excess carbon which exists on the surface as graphite or amorphous carbon) (~ 285.7 eV (C 1s)23,32 were observed, while FeO peak was not observed. The peak contributed by CrO3 (~ 579.5 eV (Cr 2p))26,27 is present only in the treated steels. The peaks associated with Cr(OH)3 (~ 578.0 eV (Cr 2p), and ~ 532.6 eV (O 1s))12,22,25,26,27 were detected in both treated and untreated steels. The peaks corresponding to Fe(OH)3 (~ 712.5 eV (Fe 2p), and ~ 532.6 eV (O 1s))27 were detected in treated steels. The complete information about peak deconvolution are reported in Supplementary material 1.
XRD patterns of 316L stainless steels treated at 300 W for 10 to 30 min and the untreated steel.
Fe 2p, Cr 2p, O 1s, and C 1s XPS spectra of 316L stainless steels treated at 300 W for 10 to 30 min and the untreated steel. The spectra (gray), convoluted peaks (black), and deconvoluted peaks (colors) are present. M in chemical formular of compound denotes Fe or Cr. The color of each deconvoluted peak corresponds to a color of dash line that indicates the position of binding energy of the chemical species.
The XRD and XPS results reveal surface morphology of steel in surface and near surface regions (by providing depth of analyses in micro- and nanoscales). For XPS results, it should be noted that Ni 2p signal was covered with background and is not present in this work. This reflects very low content of Ni in surface region and instability of Ni-containing compound in this carburizing condition. The XRD and XPS results show that the surface of untreated steel consists of a metallic bulk (solid solution of Cr in γ-Fe) which located under oxide-containing layers of Cr2O3, FeCr2O4, and FeO. Formation of FeO and FeCr2O4 generally occurs in a low chromium-content region. This region is produced by a slow diffusion of chromium at low temperature. The formation of FeCr2O4 is given by15
Fe2O3 was not detected due to possession of lower thermodynamic stability than Cr2O3 at ambient temperature34. A presence of Cr23C6 reflects a precipitation of this phase which generally observed in austenitic stainless steel and aged 316L stainless steel6. The precipitation resulted from a reaction35
The carbon-oxide compound (with binding energy corresponding to carboxyl ((CO*)OH)) observed in the spectra was due to surface contamination. Observation of hydroxides resulted from the exposure of steel to moisture as given by36
where M denotes Fe or Cr. The Fe(OH)3 peaks are proposed to be not observed in the untreated steel due to Fe(OH)3 was less stable than Cr(OH)3 when the uncarburized steel exposed to air37. The peak observed at ~ 532.6 eV (O 1s) contributed by M(OH)3 is therefore proposed to be of Cr(OH)3 located at the outermost surface of untreated steel. The results are in agreement with previous research38. For treated steels, the M2O3 formed during carburizing at high temperature via a reaction15
when the steel was exposed to humid air after carburizing, the O–M bonds of M2O3 were weakened by H2O adsorption. The O atom of H2O molecule was bonded to M atom of M2O3, and another H–O bond was broken to form hydroxyl group (OH−)39. Formation of M(OH)3 is proposed to be given by
For the steel treated for 10 min, no adding carbide produced by the carburizing process was observed at near surface by XPS. However, the nano-grain carbide was observed at a higher depth by XRD where the concentration of carbon in steel reached a critical level for Cr7C3 formation as given by35
This equation indicates higher stability of Cr7C3 (in comparison with Cr23C6) when the steel contains larger amount of carbon as reported by previous research4,23. Observation of additional Fe2O3 simultaneously with disappearance of Fe and Cr indicates oxidation of these metals which results in larger amount of oxide formation. The formation of Fe2O3 resulted from the reaction between outward-diffusing Fe2+ (through Cr2O3)40 and inward-diffusing O2− at outermost surface of steel. The reduction of peak intensity in O 1s spectrum of low oxygen containing oxide such as FeO was due to possession of lower stability of this phase than the untreated steel. The reduction reflected larger amount of oxygen content in the surface of steel treated for 10 min. The high oxygen content also resulted in oxidation of Cr2O3 to form CrO3. The formation of carbides in steel treated for 20 min resulted from the reactions between C and compounds in steels15,35,41:
The formation of Cr3C2 was difficult to be confirmed solely by XPS due to the binding energies of Cr 2p (~ 575.8 eV) and C 1s (~ 286.7 eV) for Cr3C2 are very close to other chromium carbide23,41. This carbide is proposed to be Cr23C6 which observed in uncarburized steel as described by Eq. (3). In thermodynamics theory of phase transformation, the phase existence and stability associate with formation (nucleation and growth) and decomposition of phase which can be indicated by amount of phase and grain size provided by XRD results. The XRD results show lower thermodynamic stability of Cr7C3 (indicated by the lower peak intensity and smaller grain size as described in Supplementary material 1) for the steel treated for 20 min when compared to 10 min due to some reasons. Cr7C3 in steel treated for 20 min decomposed and reacted with carbon to form Cr3C2 as given by reaction (10). The expense growth of Cr3C2 nanograins was able to suppress the Cr7C3 neighbors. The relative amount of Cr3C2 was larger than Cr7C3 after carburizing time of 20 min.The contents of Cr7C3 and Cr3C2 increased with increasing carburizing time. The results show that the highest carbon-containing carbide, Cr3C2, formed due to possession of high thermodynamics stability when chromium-containing material possessed large amount of carbon content at the suitable temperature for carbide formation. The large amount of carbon is reflected by a presence of a peak of graphite in which resulted from deposition of unreacted excess carbon. Disappearance of FeO and formation of Fe7C3 when the steels possessed high oxygen and carbon contents are proposed to be due to the reaction1,42:
Some nascent carbon (from carbon source) had not been involved in carbide formation and existed as free carbon. Some free carbon was amorphous and not seen in the XRD scan. Amount of free carbon on the steel surface tended to increase with increasing carburizing time as shown in the C 1s spectra. The steel treated for 30 min experienced the same compound formation as the 20 min with adding of ferrite. This ferrite was proposed to be the metal particles in oxide scale as reported in previous research2. These metal particles were produced by decomposition of FeCr2O4 as given by2
Carbon can diffuse through the α-Fe as an additional path. The formation of carbide was therefore attributed to a combined effect of traditional diffusion, grain boundary diffusion, and diffusion through the α-Fe particles. The XPS and XRD results therefore reveal surface morphologies of uncarburized steel and steels carburized under low oxygen-partial pressure as multilayer reported in Table 1. The multilayer of treated steels consisted of nano-grain carbide(s) generated in the compound layer that located between outermost protective layer and inner base stainless steel. The steel possessed development of phase and amount of carbide formation as carburizing time increased from 10 (Cr7C3) to 20 and 30 min (Fe7C3 + Cr7C3 + Cr3C2).
Electrochemical behavior of the steels carburized at 300 W for 10 to 30 min and the uncarburized steel was investigated using EIS. The results (Fig. 4) and parameters (Table 2) obtained by curve fitting using the equivalent circuit with two time constants43,44 are shown. EIS parameters including constant phase element (CPE)-capacitive parameter (Q), capacitance associated with the CPEs (CCPEcl and CCPEdl), passive (resistive) impedance of electrode (Z′), and α were calculated and reported. The value of α associates with microscopic surface roughness. The values of 0, 1, and –1, correspond to resistive, capacitive, and inductive behaviors, respectively45,46. Z′ is a summation of a polarization resistance of steel (Rp) and Ohmic resistance (Re). Rp is obtained by summation of chemical layer resistance (Rcl) and charge transfer resistance (Rct). CCPEcl and CCPEdl were calculated from QCPEcl, QCPEdl, Rp, and α (using normal distribution) as given by47
(a) Nyquist plots and the equivalent circuit used for simulation; (b) inset of Nyquist plots; c and d, Bode plots for 316L stainless steels carburized at 300 W for 10 to 30 min and the uncarburized steel. The EIS experimental data and simulated curves are represented by circles and lines, respectively.
The relaxation process was clarified by Faradaic impedance of electrode which was simulated using the equivalent circuit with two time constants as shown in Fig. 4a. This circuit is appropriate for fitting of experimental impedance data of 316L stainless steel obtained in aerated media44. The impedance was constituted of real (Z′) and imaginary (Z′′) components corresponding to passive (resistive) and reactive (capacitive and/or inductive) contributions, respectively. The Faradaic impedance of steel was divided into two parts: chemical layer and double layer impedances which each contributed by Z′ and Z′′. These two impedances each consist of resistance (R) and capacitive impedance of a constant phase element which is given by48
where Q, j, and ω are CPE-capacitive parameter, \(\sqrt { - 1}\) , and angular frequency, respectively. The Nyquist plots of steels in Fig. 4a,b each show one time constant that indicates one relaxation or rate determining process for each steel. The relaxation frequencies (fr) of processes were in the range of below 1 Hz which indicated the rate determining relaxation process of oxygen adsorption on electrode surface44,48. fr values for the carburized and uncarburized steels are in the order of magnitude o 0.1 and 0.01, respectively, as shown in Table 2. The adsorbed oxygen influenced on conversion and uncharged diffusion process. The conversion process associates with redox reaction that occurs in material-surface region. In redox reaction, metal atoms are oxidized and converted to metal ions and electrons. O atoms dissociated from O2 gas molecules (in electrolyte) adsorbing onto the surface are reduced by these electrons which results in generation of O2−7,49. In the testing environment of electrolyte with no carbon potential, Cr3C2 was less thermodynamically stable than Cr7C3 and underwent a larger amount of decomposition. The decomposition gave rise to the redox reaction or conversion process due to Cr3+ decomposed from the carbide was able to promote the reduction of adsorbing O atoms. The rising of redox reaction resulted in reduction of Rct of the steel treated for 20 min when compared to 10 min. The uncharged diffusion process associates with O2 diffusion (perpendicular to the surface) in a stagnant gas layer that establishes an O2 concentration gradient (producing diffusion impedance) over the surface7,50. As active species, O2 diffused down the concentration gradient which arisen between the material surface and the location from material surface where the O2 concentration equal to a bulk solution. The bulk solution outside the stagnant layer possessed the higher O2 concentration than at the material surface. However, slow dissociation of O2 on the surface (which implied slow reduction rate) resulted in the accumulation of O2 and decrease in concentration gradient which gave rise to Rct of the steel treated for 30 min. Rcl of the treated steels were lower than Rct for two orders of magnitude which indicated small contribution of migration process in the corrosion of treated steels. The migration process associates with ion migration in chemical layer, and chemical layer impedance which depends on the structure of layer including phase, amount of compound, and grain size. The higher value of Rcl (~ 4.5 times) for the steel carburized for 30 min when compared to 10 and 20 min reflected the larger contribution of chemical layer impedance as reported in literature8,51,52. The results are in agreement with previous research53. XRD results show that Cr7C3 is the major compound formed in the carburized steels. The grain size of Cr7C3 therefore influenced on migration of metal ions which was largely contributed by a preferential diffusion pathway such as grain boundary. The small grain size in steel treated for 20 min contributed to the fast diffusion which corresponded to low Rcl. However, Rcl of the steel treated for 20 min was higher than 10 min. It is proposed that the large thickness of compound layer and large grain size of Cr3C2 had some contribution in retardation of both traditional and grain-boundary diffusion in the steel treated for 20 min. The Rcl was therefore contributed by larger thickness of compound layer and grain-boundary diffusion associated with small Cr7C3 and large Cr3C2 grains. These contributions were larger than grain-boundary diffusion associated with large Cr7C3 grains in thin compound layer of the steel treated for 10 min. Even though the grain size of steel treated for 30 min was not the largest, the steel possessed the largest amount of Cr7C3 formation (as shown by XRD) and thickest compound layer (Supplementary material 2) which resulted in the highest Rcl. A deviation from semi-circle shape of the Nyquist plots shown in Fig. 4b reflects a larger contribution of resistive than a capacitive one. The resistive contribution (corresponding to Z′) was therefore the main contribution in Faradaic impedance. Besides, a capacitance calculated from QCPE was able to imply the electrochemical susceptibility of steel. CPE-capacitance of chemical layer (CCPEcl) was attributed to the accumulation of charges (metal ions)47 in chemical layer of carburized steel. The steel with high CCPEcl (such as carburized for 20 min) tended to be susceptible to corrosion. The CPE-capacitance of double layer (CCPEdl) of steels possessed different contribution in different relaxation processes. For the processes of oxygen adsorption and uncharged diffusion, high CCPEdl indicated the large amounts of adsorption and accumulation of O2 gas on steel surface. The high CCPEdl implied the slow dissociation of O2 or generation of O2− which promoted the corrosion resistance of steel. For conversion process, high CCPEdl indicated high conversion rate which promoted electrochemical susceptibility of steel. For the steel carburized for 20 min, large amounts of decomposition of Cr3C2 and reduction of adsorbing O atoms (promoted by small Cr7C3 grains) resulted in large amount of charge accumulation (of Cr3+ and O2−) in double layer which resulted in high value of CCPEdl. The contribution of Rct in passive impedance (Rp) of treated steels was larger than Rcl (for 2 orders of magnitude) as indicated by the values shown in Table 2. This reflects that oxygen adsorption had a greater effect than the migration process. The passive impedance reflecting corrosion resistance of steel therefore had an ascending order of the steel treated for 20 < 10 < 30 min. The order is in agreement with the results of potentiodynamic polarization reported in Supplementary material 3. The value of Rp for untreated steel was 1 to 2 orders of magnitude higher than the treated steels. The contribution of Rcl in Rp was larger than Rct which reflected the large contribution of protective layer for untreated steel.
The results show that formation of nano-grain carbide(s) during carburizing had deterioration effect on the electrochemical behavior of steel due to disturbance of formation (as well as self-healing) of protective layer by delaying the growth of layer to achieve the critical thickness of protection54,55. However, the steel with large amount of carbide generation (treated for 30 min) tended to have higher corrosion resistance than the smaller ones (10 and 20 min) due to some reasons. Possession of smaller amount of ion migration as indicated by higher value of Rcl, and larger amounts of adsorption and accumulation of O2 in a stagnant gas layer on surface of steel which resulted in reduction of concentration gradient and gave rise to Rct. The electrochemical behavior of carburized 316L austenitic stainless steel in this study exhibits the same trend as the 420 martensitic stainless steel of our previous work7,54 due to the formation of nano-grain-compound layer. The trend also shows some correspondence to previous research in which corrosion resistance of carburized 316L stainless steel (with formation of micro-grain-compound layer) was superior to the uncarburized steel. The enhancement of micro-grain-carburized layer resulted from retardation of mobility of oxygen-vacancy and metal-ion52,55,56. Besides, this also reflects the different electrochemical behavior between the carburized steels with nano- and micro-grain carbides. The corrosion resistance associated with electrochemical behavior of stainless steel is therefore mainly influenced by grain size, and amounts of hydroxide, oxide, and carbide formation of Cr. These compounds have an effect on determination of relaxation process of steel. For the sustainable operation of 316L stainless steel parts, the control of wet corrosion in period of formation of nano-grain carbide is highly recommended. The wet-corrosive environment and in-service period should be controlled and extended, respectively, until the nano-grain carbide has been developed to micro-grain carbide.
Carburizing of 316L stainless steel in low oxygen-partial pressure resulted in formation of surface multilayer with nano-grain carbide(s). The carbide(s) generated in the compound layer that located between outermost protective layer and inner base stainless steel. The steel underwent development of phase and amount of carbide formation as carburizing time increased from 10 (Cr7C3) to 20 and 30 min (Fe7C3 + Cr7C3 + Cr3C2). Formation of nano-grain carbide(s) during carburizing had deterioration effect on the electrochemical behavior of steel due to disturbance of formation (as well as self-healing) of protective layer by delaying the growth of layer to achieve the critical thickness of protection. However, the steel with large amount of carbide generation (treated for 30 min) tended to have higher corrosion resistance than the smaller ones (10 and 20 min) due to some reasons. Possession of smaller amount of ion migration as indicated by higher value of Rcl, and adsorption and accumulation of O2 in a stagnant gas layer on surface of steel which resulted in the reduction of O2-concentration gradient and gave rise to Rct. Phase, grain size, morphology, and amount of compound formation during carburizing had the effect on relaxation process of steel. For the sustainable operation of 316L stainless steel parts, the control of wet corrosion in period of formation of nano-grain carbide is highly recommended.
Tabet, N., Allam, I. & Yin, R. C. X-ray photoelectron spectroscopy investigation of the carburization of 310 stainless steel. Appl. Surf. Sci. 220, 259–272. https://doi.org/10.1016/S0169-4332(03)00820-1 (2003).
Article ADS CAS Google Scholar
Zeng, Z., Natesan, K., Cai, Z. & Darling, S. B. The role of metal nanoparticles and nanonetworks in alloy degradation. Nature Mater. 7, 641–646. https://doi.org/10.1038/nmat2227 (2008).
Article ADS CAS Google Scholar
Wang, Y. & Chen, W. Microstructures, properties and high-temperature carburization resistances of HVOF thermal sprayed NiAl intermetallic-based alloy coatings. Surf. Coat. Technol. 183, 18–28. https://doi.org/10.1016/j.surfcoat.2003.08.080 (2004).
Samaras, G. F. & Haidemenopoulos, G. N. Carburization of high-temperature steels: A simulation-based ranking of carburization resistance. Eng. Fail. Anal. 51, 29–36. https://doi.org/10.1016/j.engfailanal.2015.02.022 (2015).
Kaya, A. A., Krauklis, P. & Young, D. J. Microstructure of HK40 alloy after high temperature service in oxidizing/carburizing environment I. Oxidation phenomena and propagation of a crack. Mater. Charact. 49, 11–21. https://doi.org/10.1016/S1044-5803(02)00249-8 (2002).
Murr, L. E. et al. Grain boundary and microstructure engineering of Inconel 690 cladding on stainless-steel 316L using electron-beam powder bed fusion additive manufacturing. J. Mater. Sci. Technol. 35, 351–367. https://doi.org/10.1016/j.jmst.2018.09.059 (2019).
Boonruang, C., Thong-on, A. & Kidkhunthod, P. Effect of nanograin-boundary networks generation on corrosion of carburized martensitic stainless steel. Sci. Rep. 8, 2289. https://doi.org/10.1038/s41598-018-20671-z (2018).
Article ADS CAS PubMed PubMed Central Google Scholar
Wang, Q., Zhou, F., Zhou, Z., Li, L.K.-Y. & Yan, J. Influence of carbon concentration on the electrochemical behavior of CrCN coatings in simulated body fluid. Surf. Coat. Technol. 265, 16–23. https://doi.org/10.1016/j.surfcoat.2015.01.068 (2015).
Li, N. & Wang, N. The effect of duplex surface mechanical attrition and nitriding treatment on corrosion resistance of stainless steel 316L. Sci. Rep. 8, 8454. https://doi.org/10.1038/s41598-018-26844-0 (2018).
Article ADS CAS PubMed PubMed Central Google Scholar
Moteshakker, A. & Danaee, I. Microstructure and corrosion resistance of dissimilarweld-joints between duplex stainless steel 2205 and austenitic stainless steel 316l. J. Mater. Sci. Technol. 32, 282–290. https://doi.org/10.1016/j.jmst.2015.11.021 (2016).
Fernández-Domene, R. M., Blasco-Tamarit, E., García-García, D. M. & García-Antón, J. Effect of alloying elements on the electronic properties of thin passive films formed on carbon steel, ferritic and austenitic stainless steels in a highly concentrated LiBr solution. Thin Solid Films 558, 252–258. https://doi.org/10.1016/j.tsf.2014.03.042 (2014).
Article ADS CAS Google Scholar
Hermas, A. A. XPS analysis of the passive film formed on austenitic stainless steel coated with conductive polymer. Corros. Sci. 50, 2498–2505. https://doi.org/10.1016/j.corsci.2008.06.019 (2008).
Xu, N., Monceau, D., Young, D. & Furtado, J. High temperature corrosion of cast heat resisting steels in CO + CO2 gas mixtures. Corros. Sci. 50, 2398–2406. https://doi.org/10.1016/j.corsci.2008.06.001 (2008).
Alvarez, J. et al. Role of Al oxide PVD coatings in the protection against metal dusting. Surf. Coat. Technol. 204, 779–783. https://doi.org/10.1016/j.surfcoat.2009.09.060 (2009).
Hänsel, M., Boddington, C. A. & Young, D. J. Internal oxidation and carburisation of heat-resistant alloys. Corros. Sci. 45, 967–981. https://doi.org/10.1016/S0010-938X(02)00182-8 (2003).
Yu, C., Nguyen, T. D., Zhang, J. & Young, D. J. Corrosion of Fe–9Cr–(Mn, Si) alloys in CO2–H2O–SO2 gases. Corros. Sci. 98, 516–529. https://doi.org/10.1016/j.corsci.2015.05.040 (2015).
Chiu, M.-Y., Jeng, U.-S., Su, C.-H., Liang, K. S. & Wei, K.-H. Simultaneous use of small- and wide-angle X-ray techniques to analyze nanometerscale phase separation in polymer heterojunction solar cells. Adv. Mater. 20, 2573–2578. https://doi.org/10.1002/adma.200703097 (2008).
Chen, Z. W. et al. Microstructural evolution of oxides and semiconductor thin films. Prog. Mater. Sci. 56, 901–1029. https://doi.org/10.1016/j.pmatsci.2011.02.001 (2011).
Kondo, T. et al. Size dependent lattice constant change of thiol self-assembled monolayer modified Au nanoclusters studied by grazing incidence X-ray diffraction. Electrochem. Commun. 65, 35–38. https://doi.org/10.1016/j.elecom.2016.02.007 (2016).
Feng, K., Wang, Y., Li, Z. & Chu, P. K. Characterization of carbon ion implantation induced graded microstructure and phase transformation in stainless steel. Mater. Charact. 106, 11–19. https://doi.org/10.1016/j.matchar.2015.04.019 (2015).
Wang, S.-C., Lin, H.-T., Nayak, P. K., Chang, S.-Y. & Huang, J.-L. Carbothermal reduction process for synthesis of nanosized chromium carbide via metal-organic vapor deposition. Thin Solid Films 518, 7360–7365. https://doi.org/10.1016/j.tsf.2010.05.001 (2010).
Article ADS CAS Google Scholar
Lu, C.-E., Pu, N.-W., Hou, K.-H., Tseng, C.-C. & Ger, M.-D. The effect of formic acid concentration on the conductivity and corrosion resistance of chromium carbide coatings electroplated with trivalent chromium. Appl. Surf. Sci. 282, 544–551. https://doi.org/10.1016/j.apsusc.2013.06.008 (2013).
Article ADS CAS Google Scholar
Castillejo, F. E., Marulanda, D. M., Olaya, J. J. & Alfonso, J. E. Wear and corrosion resistance of niobium-chromium carbide coatings on AISI D2 produced through TRD. Surf. Coat. Technol. 254, 104–111. https://doi.org/10.1016/j.surfcoat.2014.05.069 (2014).
Ghods, P., Isgor, O. B., Brown, J. R., Bensebaa, F. & Kingston, D. XPS depth profiling study on the passive oxide film of carbon steel in saturated calcium hydroxide solution and the effect of chloride on the film properties. Appl. Surf. Sci. 257, 4669–4677. https://doi.org/10.1016/j.apsusc.2010.12.120 (2011).
Article ADS CAS Google Scholar
Cao, X. Y., Ding, X. F., Lu, Y. H., Zhu, P. & Shoji, T. Influences of Cr content and PWHT on microstructure and oxidation behavior of stainless steel weld overlay cladding materials in high temperature water. J. Nucl. Mater. 467, 32–41. https://doi.org/10.1016/j.jnucmat.2015.09.015 (2015).
Article ADS CAS Google Scholar
Biesinger, M. C. Resolving surface chemical states in XPS analysis of first row transition metals, oxides and hydroxides: Cr, Mn, Fe, Co and Ni. Appl. Surf. Sci. 257, 2717–2730. https://doi.org/10.1016/j.apsusc.2010.10.051 (2011).
Article ADS CAS Google Scholar
Ningshen, S., Sakairi, M., Suzuki, K. & Ukai, S. The passive film characterization and anodic polarization behavior of 11% Cr ferritic/martensitic and 15% Cr oxide dispersion strengthened steels in different electrolytic solutions. Appl. Surf. Sci. 274, 345–355. https://doi.org/10.1016/j.apsusc.2013.03.059 (2013).
Article ADS CAS Google Scholar
Abdel-Samad, H. & Watson, P. R. An XPS study of the adsorption of chromate on goethite (α-FeOOH). Appl. Surf. Sci. 108, 371–377. https://doi.org/10.1016/S0169-4332(96)00609-5 (1997).
Article ADS CAS Google Scholar
Kettle, J., Ding, Z., Horie, M. & Smith, G. C. XPS analysis of the chemical degradation of PTB7 polymers for organic photovoltaics. Org. Electron. 39, 222–228. https://doi.org/10.1016/j.orgel.2016.10.016 (2016).
Smith, M., Scudiero, L., Espinal, J., McEwen, J.-S. & Garcia-Perez, M. Improving the deconvolution and interpretation of XPS spectra from chars by ab initio calculations. Carbon 110, 155–171. https://doi.org/10.1016/j.carbon.2016.09.012 (2016).
Kwan, Y. C. G., Ng, G. M. & Huan, C. H. A. Identification of functional groups and determination of carboxyl formation temperature in graphene oxide using the XPS O 1s spectrum. Thin Solid Films 590, 40–48. https://doi.org/10.1016/j.tsf.2015.07.051 (2015).
Article ADS CAS Google Scholar
Wang, Y.-J., Fang, B., Li, H., Bi, X. T. & Wang, H. Progress in modified carbon support materials for Pt and Pt-alloy cathode catalysts in polymer electrolyte membrane fuel cells. Prog. Mater. Sci. 82, 445–498. https://doi.org/10.1016/j.pmatsci.2016.06.002 (2016).
Groudeva-Zotova, S., Vitchev, R. G. & Blanpain, B. Phase composition of Cr–C thin films deposited by a double magnetron sputtering system. Surf. Interface Anal. 30, 544–548. https://doi.org/10.1002/1096-9918(200008)30:1%3c544::AID-SIA814%3e3.0.CO;2-7 (2000).
Wicks, C. E. & Block, F. E. Thermodynamic Properties of 65 Elements—Their Oxides, Halides, Carbides, and Nitrides. (United State Government Printing Office, Washington, 1963, pp. 34 & 58).
Young, D. J. Simultaneous oxidation and carburisation of chromia forming alloys. Int. J. Hydrog. Energy 32, 3763–3769. https://doi.org/10.1016/j.ijhydene.2006.08.027 (2007).
Jones, D. A. Principles and Prevention of Corrosion. 2nd ed. (Macmillan Pub. Co., New York, 1992, pp. 58).
Detriche, S. et al. XPS fast depth profile of the native oxide layers on AISI 304, 316 and 430 commercial stainless steels and their evolution with time. J. Electron Spectrosc. Relat. Phenom. 243, 146970. https://doi.org/10.1016/j.elspec.2020.146970 (2020).
Lothongkum, G., Chaikittisilp, S. & Lothongkum, A. W. XPS investigation of surface films on high Cr-Ni ferritic and austenitic stainless steels. Appl. Surf. Sci. 218, 202–209. https://doi.org/10.1016/S0169-4332(03)00600-7 (2003).
Article ADS CAS Google Scholar
Chen, C. et al. DFT study on the interaction of H2O and O2 with α-Fe2O3 (001) surface. Vacuum 188, 110164. https://doi.org/10.1016/j.vacuum.2021.110164 (2021).
Article ADS CAS Google Scholar
Birks, N., Meier, G. H. & Pettit, F. S. Oxidation of alloys, in: Introduction to the High-Temperature Oxidation of Metals, 2nd ed. (Cambridge University Press, Cambridge, UK, 2006, pp.101–162).
Zhao, Z. & Hu, W. Synthesis and characterization of chromium carbide nanopowders processed by mechanical alloying assisted microwave heating route. Int. J. Refract. Met. Hard Mater. 58, 206–210. https://doi.org/10.1016/j.ijrmhm.2016.05.003 (2016).
Bataleva, Yu. V., Palyanov, Yu. N., Borzdov, Yu. M., Bayukov, O. A. & Sobolev, N. V. Conditions for diamond and graphite formation from iron carbide at the P-T parameters of lithospheric mantle. Russ. Geol. Geophys. 57(1), 176–189. https://doi.org/10.1016/j.rgg.2016.01.012 (2016).
Wang, N., Fu, W., Zhang, J., Li, X. & Fang, Q. Corrosion performance of waterborne epoxy coatings containing polyethylenimine treated mesoporous-TiO2 nanoparticles on mildsteel. Prog. Org. Coat. 89, 114–122. https://doi.org/10.1016/j.porgcoat.2015.07.009 (2015).
Marcelin, S., Pébère, N. & Régnier, S. Electrochemical characterisation of a martensitic stainless steel in a neutral chloride solution. Electrochim. Acta 87, 32–40. https://doi.org/10.1016/j.electacta.2012.09.011 (2013).
Brug, G. J., Van Den Eeden, A. L. G., Sluyters-Rehbach, M. & Sluyters, J. H. The analysis of electrode impedances complicated by the presence of a constant phase element. J. Electroanal. Chem. 176, 275–295. https://doi.org/10.1016/S0022-0728(84)80324-1 (1984).
Harrington, S. P. & Devine, T. M. Analysis of electrodes displaying frequency dispersion in Mott-Schottky tests. J. Electrochem. Soc. 155(8), C381–C386. https://doi.org/10.1149/1.2929819 (2008).
Mahato, N., Banerjee, A., Gupta, A., Omar, S. & Balani, K. Progress in material selection for solid oxide fuel cell technology: A review. Prog. Mater. Sci. 72, 141–337. https://doi.org/10.1016/j.pmatsci.2015.01.001 (2015).
Hirschorn, B. et al. Determination of effective capacitance and film thickness from constant-phase-element parameters. Electrochim. Acta 55, 6218–6227. https://doi.org/10.1016/j.electacta.2009.10.065 (2010).
Primdahl, S. & Mogensen, M. Gas Conversion Impedance: A test geometry effect in characterization of solid oxide fuel cell anodes. J. Electrochem. Soc. 145, 2431–2438. https://doi.org/10.1149/1.1838654 (1998).
Article ADS CAS Google Scholar
Primdahl, S. & Mogensen, M. Gas diffusion impedance in characterization of solid oxide fuel cell anodes. J. Electrochem. Soc. 146, 2827–2833. https://doi.org/10.1149/1.1392015 (1999).
Article ADS CAS Google Scholar
Lin, C. H. & Duh, J. G. Electrochemical impedance spectroscopy (EIS) study on corrosion performance of CrAlSiN coated steels in 3.5 wt.% NaCl solution. Surf. Coat. Technol. 204, 784–787. https://doi.org/10.1016/j.surfcoat.2009.09.059 (2009).
Yoo, J.-H., Ahn, S.-H., Kim, J.-G. & Lee, S.-Y. Influence of target power density and substrate bias voltage on the electrochemical properties of type 304 SS films prepared by unbalanced magnetron sputtering. Surf. Coat. Technol. 157, 47–54. https://doi.org/10.1016/S0257-8972(02)00132-9 (2002).
Niu, W., Lillard, R. S., Li, Z. & Ernst, F. Properties of the passive film formed on interstitially hardened AISI 316L stainless steel. Electrochim. Acta 176, 410–419. https://doi.org/10.1016/j.electacta.2015.06.102 (2015).
Thong-on, A. & Boonruang, C. Surface modification of low carbon martensitic stainless steel by current heating technique in graphite. Surf. Coat. Technol. 306, 267–271. https://doi.org/10.1016/j.surfcoat.2016.06.034 (2016).
Heuer, A. H. et al. Enhanced corrosion resistance of interstitially hardened stainless steel: Implications of a critical passive layer thickness for breakdown. Acta Mater. 60, 716–725. https://doi.org/10.1016/j.actamat.2011.10.004 (2012).
Article ADS CAS Google Scholar
Adachi, S. & Ueda, N. Surface hardness improvement of plasma–sprayed AISI 316L stainless steel coating by low-temperature plasma carburizing. Adv. Powder Technol. 24, 818–823. https://doi.org/10.1016/j.apt.2012.12.011 (2013).
This study was supported by Center of Excellence in Materials Science and Technology, Chiang Mai University. We thank to Department of Physics, Faculty of Science, Srinakharinwirot University for providing EIS and PP measurements.
Department of Physics and Materials Science, Faculty of Science, Chiang Mai University, Chiang Mai, 50200, Thailand
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Center of Excellence in Materials Science and Technology, Chiang Mai University, Chiang Mai, 50200, Thailand
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C.B. conceived the idea, designed the study, supervised the research, performed XRD and XPS, helped in EIS and PP measurements, fitted data, analyzed, interpreted and discussed all results, prepared all figures, and wrote the manuscript. W.S. prepared the samples and performed EIS and PP measurements.
The authors declare no competing interests.
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Boonruang, C., Sanumang, W. Effect of nano-grain carbide formation on electrochemical behavior of 316L stainless steel. Sci Rep 11, 12602 (2021). https://doi.org/10.1038/s41598-021-91958-x
DOI: https://doi.org/10.1038/s41598-021-91958-x
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