Effects of Deposition Potentials on the Morphology and Structure of Iron-Based Films on Carbon Steel Substrate in an Alkaline Solution

The purpose of this work is to investigate the effect of electrochemical deposition potential on the morphology and structure of iron-based films on the carbon steel in an alkaline Fe(III)-triethanolamine solution.The deposition potentials were controlled in the range from −1.05 to −1.23VSCE for 1800 s at 80 C. Total amount of electric charge for electrodeposition process was increased with increasing deposition potential in negative direction. Puremagnetite filmswith a columnar and defect-free structurewere deposited in the potential range from−1.05VSCE to −1.11 VSCE. However, petal-likemagnetite film containing ferrihydrite and ironwas formed at−1.17 VSCE. Atmore negative potential of−1.23 VSCE, two distinct layerswere observed: a porous outer layer containing ferrihydrite and goethite and a compact inner layer consisting of columnar metallic iron. In the potential range from −1.05 to −1.11 VSCE, the pure magnetite films gradually increased the thickness and decreased the surface roughness with an increase of the overpotential. The magnetite film deposited at −1.11 VSCE showed the most thick layer and smooth surface state.


Introduction
Magnetite is one of the principal corrosion products formed on the carbon steel surfaces of piping and equipment of the secondary coolant system in pressurized water reactor (PWR) of nuclear power plant.Magnetite is released from carbon steel surfaces into the high temperature feed water and is transported to the steam generator [1,2].Flow accelerated corrosion (FAC) leads to wall thinning of carbon steel piping and components exposed to flowing water or wet steam in the secondary system of PWR.The process of FAC is related to the dissolution of magnetite on the surface of carbon steel under turbulent flow [3,4].In addition, magnetite deposits on the outside of the steam generator tubes and tube support structure.There has been an intense interest in magnetite deposits on the nuclear materials because its removal improves heat transfer and reduces the corrosion of steam generator tube and other parts of the steam generator system [5,6].In order to evaluate the corrosion behavior of the magnetite covering the nuclear materials, a rigid method to deposit magnetite on the corresponding material substrates should be established.Therefore, it is of high interest to find a simple and efficient method to produce the magnetite film.
Recently, electrodeposition method has extensively been investigated to produce magnetite films [7][8][9][10][11][12].There are two basic approaches to deposit the magnetite by anodic deposition in Fe(II) systems [7][8][9][10] and cathodic deposition in Fe(III) systems [11,12].Most of the previous work was conducted in the Fe(II) systems, where Fe(II) ions were complexed with organic compounds and were electrochemically oxidized to form magnetite film in an inert atmosphere at an elevated temperature.A problem with this method is that the complexed Fe(II) can be oxidized by molecular oxygen in the air; thus special attention must be paid to exclude molecular oxygen.
Sapieszko and Matijević [13] developed the hydrothermal method to produce the magnetite powder in Fe(III)triethanolamine (TEA) solution agents.Switzer's group have modified the Fe(III)-TEA solution and developed the efficient 2 Advances in Materials Science and Engineering method to produce the magnetite film on the stainless steel substrate [14], single crystal Au [15], and Ni [16] at 80 ∘ C.This method is not necessary to eliminate molecular oxygen from the deposition environment due to the good stability of Fe(III)-TEA complex [14][15][16].Recently, Switzer's group showed that the polycrystalline magnetite films electrodeposited on stainless steels exhibit multistate resistance switching and resistance switching can be tuned by controlling the composition of the films by varying the deposition potential [17,18].Goujon et al. [19,20] showed the characterization of magnetite films electrodeposited on the Ni-based alloys and established the optimal temperature and agitation condition for electrodeposition to grow magnetite films in the Fe(III)-TEA solution.Duan et al. [21] also presented that the concentration of Fe(III) ions had an impact on the electrodeposition rate, while the deposition temperature and time strongly affected the morphology of the magnetite films.
However, there is a few researches for the electrodeposition of iron-based films on the carbon steel substrate in the Fe(III)-TEA solution.In particular, the effect of deposition potentials on the morphology, structure, thickness, and surface roughness of the electrodeposited films on the carbon steel substrate has not been verified.
The aim of this study is to elucidate the effects of deposition potential on the morphology, structure, thickness, and surface roughness of the electrodeposited films on the carbon steel in Fe(III)-TEA solution, thus establishing the optimal deposition potential to form dense and thick magnetite films.It is considered that these results are useful for simulating the deposited corrosion products on the surface of carbon steel materials in the secondary system of nuclear power plant.

Material Preparation.
Carbon steel specimens for magnetite deposition were machined into 10 × 5 × 1 mm from the SA106Gr.B pipe material.The carbon steel substrates were mechanically ground up to #1100 grit silicon carbide paper and then ultrasonically cleaned in acetone and deionized water.The chemical composition of SA106Gr.B is given in Table 1.

Electrodeposition of Films.
The iron-based films were electrodeposited from an alkaline solution of Fe 2 (SO 4 ) 3 complexed with TEA.The deposition bath for magnetite was prepared by dissolving 26 g of Fe(III) sulfate hydrate in 150 mL of 1 M TEA.It was diluted with 500 mL of deionized water.The solution was then added to a second solution of 120 g of NaOH pellets in 850 mL of deionized water.The resulting deposition solution was gray-green colored with pH 12.5 at 25 ∘ C.
The electrochemical deposition was carried out in a three-electrode cell.A saturated calomel electrode (SCE) and a platinum wire were used as the reference and counter electrode, respectively.During the deposition process, the solution was maintained at 80 ∘ C and stirred at 200 rpm.The deposition potentials were as follows: −1.05 V SCE , −1.08 V SCE , −1.11 V SCE , −1.17 V SCE , and −1.23 V SCE .The electrodeposition time was 1800 s at all the deposition potentials.To ensure a deposition as homogeneous as possible, the carbon steel substrate was fixed in front of the counter electrode.After electrodeposition, the electrodeposited films were carefully rinsed with deionized water and dried in air.

Characterization of Electrodeposited Films.
The electrodeposited films were analyzed by scanning electron microscope-energy dispersive X-ray spectroscopy (SEM-EDS) and X-ray diffraction (XRD).In order to analyze the morphology, thickness, and chemical composition of the electrodeposited films on the carbon steel substrate, the electrodeposited films were milled by a focused ion beam (FIB) toward a vertical direction of the electrodeposited films.Adherence of electrodeposited films was confirmed by FIB-SEM.The values of the surface roughness were measured using a noncontacting surface profiler.In this paper, the root mean square roughness (  ) is used.The thickness and roughness of electrodeposited films were measured at least three times to confirm the reproducibility.The values were presented by the average with error bars, and good reproducibility was confirmed.
The chemical species of the electrodeposited films were analyzed using X-ray photoelectron spectroscopy (XPS).An XPS analysis was carried out using a Thermo Fisher Scientific (Theta Probe AR-XPS) X-ray photoelectron spectrometer with an Al K X-ray source (1486.6 eV) operated at 15 kV and 150 W under a base pressure of 2.7 × 10 −7 Pa.The binding energies of all peaks were corrected by the reference C 1s peak at 284.5 eV.The electrodeposition of magnetite film in Fe(III)-TEA solution can be simplified by two steps.The first step is that the Fe(III)-TEA solution is electrochemically reduced to an Fe(II)-TEA complex.The reaction, which may occur, is expressed as reaction (1).The second step is that Fe(III)-TEA complex would then chemically react with Fe(II)-TEA to produce magnetite at the surface of the substrate in the following reaction (2).The overall electrochemical reaction leading to the formation of magnetite deposit on the substrate is reaction (3).The proposed mechanism is expressed in the following reactions (1) to (3) [14][15][16][17][18]:

Electrodeposition of the Films.
Therefore, the first reduction wave observed between −0.95 and −1.20 V SCE can be attributed to a one electron reaction corresponding to the above reaction (1) [14,17].On the contrary, the second reduction wave between −1.20 and −1.30V SCE seems to be due to a two-electron process corresponding to the reduction of Fe(II) to Fe [15][16][17][18].
Figure 2 shows the surface morphologies of the films formed at different deposition potentials.It is obvious that the morphology depends on the electrochemical potential.The films deposited at −1.05 and −1.08 V SCE have highly faceted morphologies (Figures 2(a) and 2(b)).In this range of potentials, the degree of faceting and particle size of the deposits decrease as the overpotential increases, whereas the film formed at −1.11 V SCE is flat morphologies (Figure 2(c)).As shown in Figure 2(d), the film deposited at −1.17 V SCE has a petal-like microstructure.The film deposited at −1.23 V SCE is similar to that deposited at −1.17 V SCE (Figure 2(e)).These morphologies of the five films are homogeneous on the whole surface of the deposits.
At low overpotentials (−1.05, −1.08, and −1.11), the surface concentration of Fe(III) is nearly the same as the bulk concentration because the ion diffusion is sufficient.Hence, the structure is determined by the preferential growth of favorably oriented crystal faces.As a result, the deposited film formed transforms to a dense and crack-free morphology with tightly packed, well-faceted crystallites.Whereas at high overpotentials (−1.17, −1.23 V SCE ) the current becomes masstransport controlled, the surface concentration of Fe(III) approaches zero because the ion diffusion is insufficient.As a result, the resultant structure is dominated by open boundaries and the deposit exhibits a petal-like structure.
Figure 3 shows the FIB-SEM images on a cross section of the electrodeposited films.The films deposited in a range from −1.05 to −1.11 V SCE grew with a columnar morphology.The columns are very compact and adherent to the carbon steel substrate.No defects such as hole, gap, and crack can also be observed at the interface between the deposited films and carbon steel substrate, which confirms that the deposited films are tightly bonded to carbon steel substrate.However, the film deposited at −1.17 V SCE shows a very defective structure containing numerous holes and gaps, indicating that the deposited films are bonded weakly to the carbon steel substrate.The film deposited at −1.23 V SCE consists of two distinct layers: a porous external layer and a compact columnar inner layer.The numerous defects are observed in the external layer, similar to the film at −1.17 V SCE .However, no defects such as hole and gap can be observed in the columns and at the interface between the inner layer and carbon steel substrate.The porous cross-sectional structure of the films formed at −1.17 V SCE and −1.23 V SCE is well consistent with the top view images shown in Figures 2(d) and 2(e).
Additional analysis was performed to evaluate the double layer observed from the film deposited at −1.23 V SCE .Figure 4 shows the EDS element profile.Only iron without oxygen was detected in the inner columnar layer and the content of iron gradually increased as departing from the interface.It is therefore believed that the inner layer is composed of pure metallic iron.

Characterization of the Deposited Films.
Figure 5 shows the XRD patterns of the deposited films at the various deposition potentials.In the range from −1.05 to −1.11 V SCE , the XRD pattern shows that deposited films are all crystalline and only have peaks corresponding to magnetite.The very weak iron peak from the film at −1.08 V SCE is probably originated from the carbon steel substrate.The intensity of magnetite diffraction peaks is almost equivalent.At the electrodeposition potential of −1.17 V SCE , new XRD peaks corresponding to ferrihydrite and iron appeared, indicating the formation of a mixture of three structures: magnetite, ferrihydrite, and iron.When the electrodeposition potential has been moved to −1.23 V SCE , additional XRD peak was detected and indexed to goethite.It should be noted that the peak intensity of iron became higher than that of magnetite.Consequently, this film consisted of a mixture of complex phases: magnetite, ferrihydrite, goethite, and iron.The above XRD results indicate that the deposition potential strongly affects not only the morphology but also the structure of the deposited films.
The detection of metallic iron is in good agreement with the observation of the inner column layer consisting of metallic iron shown in Figure 4. Ferrihydrite was also detected by Mossbauer spectroscopy and XRD on the films deposited in the same electrochemical solution [15,19].However, goethite and metallic iron were not reported.Since the driving force for reduction became larger at more negative  potential, Fe(III) in the solution can be reduced to metallic iron.In addition to the reduction force, the mass transfer rate of Fe(II) in the solution to the substrate will be fast at more negative potential.This will increase the deposition rate of magnetite through reactions ( 1) and (2).Consequently, the presence of ferrihydrite and goethite is unexpected at a lower electrochemical potential.Although the formation of ferrihydrite can be attributed to the aerial oxidation of a film in basic conditions [15], further study is needed.
Figure 6 shows Fe 2p and O 1s XPS spectra of the films deposited at the various potentials.As shown in Figure 6(a), Fe 2p core levels were split into 2p 3/2 and 2p 1/2 doublet.The binding energy of Fe 2p 3/2 and Fe 2p 1/2 of the film deposited at −1.05 V SCE was 710.8 and 724.0 eV, respectively, which is in good agreement with the reported values for Fe 3 O 4 [22,23].However, the peak positions for Fe 2p 1/2 and Fe 2p 3/2 slightly shifted to the higher binding energy side with an increase of the overpotential.This indicates an increase in the proportion of Fe(III) species in the films.The binding energy of ferrihydrite and goethite is higher than that of pure magnetite [24,25].Therefore, the shift of the peak positions to the higher binding energy is attributed to the formation of ferrihydrite and goethite.The binding energies of O 1s are found at 530.0 eV corresponding to O 2− bonds and at 531.1 eV corresponding to OH − bonds (Figure 6(b)).In the O 1s spectrum, the film deposited at −1.23 V SCE has its maximum at 531.1 eV due to OH − bonds.This is well consistent with the XRD analysis shown in Figure 4.It should be noted that the above Fe 2p spectra represent the chemical states of the outermost surface film, because the spectra were obtained without sputtering.Therefore, the above XPS results do not entirely reflect the XRD analysis.
Figure 7 shows the thickness variation of the deposited films with the deposition potentials.The thickness of the deposited films gradually increased with an increase of the overpotential in the range from −1.05 to −1.17 V SCE , whereas the thickness sharply decreased at −1.23 V SCE .The largest thickness of the deposited film at −1.17 V SCE was about 33.2 m.The double layered films at −1.23 V SCE consisted of about 4.6 m of the porous external film and about 4.6 m of the compact inner film for a total of about 8.1 m.
Figure 8 shows the variation of deposition current density at each potential during the deposition.It is clear that the more negative deposition potential is, the higher current density is, resulting in a thick film.In particular, the abrupt Intensity (a.u.)

Fe 2p
Fe 2p 1/2 Fe 2p 3/2 730 725 720 715 710 705 735 Binding energy (eV)  increase of the film at −1.17 V SCE can be attributed to 2dimensional growth perpendiculars to the substrate and the resulting porous structure as shown in Figures 2(d) and 3(d).
Comparing the thickness of the films, the film deposited at −1.23 V SCE is thinner than that deposited at −1.11 V SCE , although the current density at −1.23 V SCE is about three times higher than that at −1.11 V SCE .This is because the three electrons are consumed to reduce Fe(III) ion to a metallic ion.
Figure 9 shows the electrodeposition charge was measured at the various potentials during electrochemical deposition.Total amount of electric charge was increased with increasing deposition potential in negative direction.
Figure 10 shows the surface roughness of films on the carbon steel substrate deposited at the various potentials using a noncontacting surface profiler.The roughness variation of  films is well associated with the surface morphology of the films shown in Figure 2. The roughness of the deposited films gradually decreased with an increase of the overpotential in the range from −1.05 to −1.11 V SCE due to the decrease of particle size.The steep increase in the roughness at −1.17 V SCE is owing to the porous petal-like morphology.At the deposition potential of −1.23 V SCE , the roughness decreased in accordance with the more dense surface morphology of the film.As shown in Figure 11, the value of   of the deposited films on the carbon steel substrate is obtained from the surface roughness curve.The surface roughness value of the deposited films at −1.11 V SCE was the smallest with 0.06 m.
Based on the results obtained in this work, it is confirmed that the electrochemical potentials affect the morphology, structure, thickness, and surface roughness of the deposited films.
In actual secondary system of nuclear power plants, porous magnetite is the main corrosion product formed on the surface of carbon steel piping, steam generator tubing, and other support structures due to the alkaline and reducing condition.Though the corrosion products are mainly made of magnetite, other corrosion products such as ferrihydrite and goethite are also present [26].And thickness of real corrosion products on carbon steel piping, steam generator tubing, and other support structures exceeds several tens of micrometers.The film deposited at −1.17 V SCE has porous morphology and several tens of micrometers thickness.Furthermore, this film contains the magnetite and ferrihydrite like the actual corrosion products in secondary system of nuclear power plants.Based on these results, the deposition potential at −1.17 V SCE is appropriate to simulate the real corrosion products formed in the secondary system of nuclear power plants.However, the deposition potential range from −1.05 V SCE to −1.11 V SCE is proper deposition condition to use specimens for the electrochemical tests due to the formation of pure adhesive homogeneous magnetite.In this range, the film deposited at −1.11 V SCE showed the most thick layer and smooth surface state.Therefore, the optimal potential for the electrodeposition of pure magnetite on the carbon steel substrate was determined to be −1.11V SCE .
To simulate the electrochemical corrosion behavior of the magnetite covering the materials, a rigid method to deposit magnetite on the corresponding material substrates should be established.In this respect, it is considered that these results are useful for simulating the deposited magnetite on the surface of carbon steel materials in the secondary system.

Conclusions
Magnetite films were electrodeposited on carbon steel substrate at different potentials in Fe(III)-TEA solution at 80 ∘ C. The electrochemical potentials affected the morphology, structure, thickness, and surface roughness of the deposited films.Pure magnetite films with a compact and defect-free structure were electrodeposited in the potential range from −1.05 V SCE to −1.11 V SCE .Porous magnetite film containing ferrihydrite and iron was obtained at −1.17 V SCE .At a more negative potential at −1.23 V SCE , double layered film was formed: a porous outer layer containing ferrihydrite and goethite and an inner columnar layer consisting of metallic iron.Based on these results, the optimal potential for the electrodeposition of pure magnetite was determined to be −1.11V SCE .These results are useful to prepare magnetite specimens for the electrochemical corrosion tests of magnetite itself and materials in contact with magnetite.

Figure 1
shows linear sweep voltammogram of the carbon steel substrate in the Fe(III)-TEA bath at 80 ∘ C. The potential was swept from the open circuit potential to −1.30 V SCE at a scan rate of 10 mV/s.The electrochemical reduction of Fe(III)-TEA started at potentials more negative than −0.95 V SCE .The first reduction wave of this linear sweep was measured approximately between −0.95 and −1.20 V SCE .The second reduction wave was also observed in the potential range from −1.20 to −1.30 V SCE .

Figure 1 :
Figure 1: Linear sweep voltammogram of the carbon steel substrate in Fe(III)-TEA solution at 80 ∘ C.

Figure 6 :Figure 7 : 2 )Figure 8 :Figure 9 :
Figure 6: XPS spectra of the electrodeposited films on the carbon steel substrate at the various potentials in Fe(III)-TEA solution for 1800 s at 80 ∘ C: (a) Fe 2p and (b) O 1s.

Figure 10 :
Figure 10: Surface roughness profile of electrodeposited films on the carbon steel substrate at the various deposition potentials in the Fe(III)-TEA solution for 1800 s at 80 ∘ C.

Figure 11 :
Figure 11: Surface roughness of the electrodeposited films on the carbon steel substrate at the various deposition potentials in Fe(III)-TEA solution for 1800 s at 80 ∘ C.