Introduction

Marine resources are rich, but the environment is complex and changeable, so many problems will be encountered in the process of marine development, and one of the most serious problems is marine corrosion. In marine engineering construction, 304SS is widely used because of its corrosion resistance. However, the high concentration of Cl- in seawater makes 304SS prone to pitting corrosion, which leads to safety accidents. The traditional corrosion protection methods of 304SS include organic polymer coating, multi-layer composite coating, electrochemical cathodic protection, etc.1,2,3, but these technologies have the problems of high cost, short service life and environmental pollution. In recent years, more and more attention has been paid to photoelectrochemistry cathodic protection by coupling n-type semiconductors with metal materials.

The new photoelectrochemistry cathodic protection technology can improve the corrosion resistance of metal corrosion environment by converting solar energy into electrochemical energy, and in terms of material anti-corrosion, it has the advantages of strong operability, cleaning, resource saving and no power consumption. The application of semiconductor materials in the field of photoelectrochemical cathodic protection needs to meet certain conditions. Firstly, the conduction band potential of semiconductors must be lower than the self etching potential in the same solution; secondly, the band gap of semiconductors should not be too wide; thirdly, the photogenerated electron–hole pairs of semiconductors are easy to separate and have low recombination rate.

TiO2 is an n-type semiconductor material with excellent photoelectric performance, stable physical and chemical properties, low toxicity, rich resources and low manufacturing cost, and it has been widely used in the field of photoelectrochemistry cathodic protection4,5,6,7,8. However, the band gap of TiO2 is wide (3.2 eV), which can only absorb ultraviolet light with wavelength less than 378 nm, and has a low utilization rate of visible light; moreover, the electron–hole pair excited by light is easy to compound, and the efficiency of light quantum is low; furthermore, TiO2 can not play the role of photoelectrochemistry cathodic protection9 under dark conditions. Therefore, modification is an important research direction to improve the photoelectric conversion performance of TiO2. The modification methods of TiO2 mainly include: metal element doping (Ni10, Fe11, Zn12), nonmetallic element doping (N13, S14), and narrow band gap semiconductor sensitization (CdTe/TiO215, CdSe/TiO216, ZnSe/TiO217, Bi2S3/TiO218) and so on. Through modification, not only the band gap width of TiO2 can be reduced, but also the separation efficiency and photoelectrochemical properties of electron hole pairs can be improved, so as to improve the photoelectrochemistry cathodic protection effect of 304SS19.

FeS2 is widely distributed in nature, mainly in the form of hematite and pyrite. Hematite type has no photoelectric property, while it will change to pyrite type when the temperature exceeds 350 °C; pyrite FeS2 is a kind of non-toxic, stable physical and chemical properties, low cost, easy to obtain semiconductor materials, and it has appropriate band gap width (0.95 eV indirect band gap, 1.03 eV direct band gap width), and high light absorption coefficient (6 × 10–5 cm−1)20, which make FeS2 is useful for the preparation of optical devices that can utilize visible light. Han21 et al. prepared wormlike FeS2/TiO2 nanotube composites, which were used for photocatalytic reduction of CO2 to methanol under visible light, and the doping and recombination of FeS2 nanoparticles on TiO2 nanotubes not only broadened the light absorption range of TiO2, but also improved the photocatalytic reduction ability, which increased the methanol yield to 91.7 μmol/h/L. Rashid22 and others prepared stable anatase TiO2 composite pyrite FeS2 composite nanocrystals to improve the photocatalytic decomposition of methyl blue, and the catalytic decomposition of organic compounds increased from 15 to 75 mg/L within 180 min. C Mutalik23 et al. successfully prepared heterostructured TiO2-FeS2 nanocomposites (NCs) by a facile solution approach to enhance light-induced antibacterial activity over a broader absorption range, and the result showed that TiO2-FeS2 NCs had better antibacterial activity than that of only TiO2 nanoparticles (NPs) or only FeS2 NPs, which suggests that TiO2-FeS2 NCs with superior light-induced antibacterial activity could be a promising antibacterial agent against bacterial infections. Li et al.24 prepared FeS2 nanoparticles by a simple hydrothermal method. The FeS2 nanoparticles obtained by reducing FeCl3·6H2O with C5H10NS2Na·3H2O were assembled on nickel foam as the anode and C nanoparticles as the cathode, and then placed together in a double-electrode alkaline electrolytic cell. Kuo25 and others prepared a kind of clean hydrogen production based on TiO2 and environmentally friendly light catalyst by wet chemical synthesis method. The catalyst is composed of FeS2–TiO2 heterostructure nanocrystals, and its absorption range is wide, which can be extended from UV–Vis spectrum to near-infrared spectrum. A wider absorption wavelength range can improve the photocatalytic hydrogen production rate. Xin et al.26 prepared photoanode materials by sensitizing TiO2 nanotubes with FeS2 of pyrite. Due to the heterogeneous structure formed at the interface between FeS2 and TiO2, the recombination rate of photogenerated electron–hole pairs was reduced, and the light absorption capacity of TiO2 increased from the ultraviolet region to the near-infrared region, thus improving the photochemical properties of composite nanomaterials.

However, there is no report on the application of FeS2 particles modified TiO2 composite nanotube arrays for photoelectrochemical cathodic protection of 304SS. In this study, FeS2/TiO2 nanocomposite films were prepared by electrochemical anodization and hydrothermal methods to improve the optical absorption capacity of TiO2 in visible light and the photoelectrochemical cathodic protection performance, and the protection mechanism for 304SS has also been studied.

Material and methods

Preparation of TiO2 nanotube array films

Firstly, cut the industrial titanium plate (20 mm × 10 mm × 0.3 mm) with purity greater than 99.6%, and ultrasonic cleaning with acetone, absolute ethanol and ultrapure water for 10 min, separately, then make a mixture of 0.9 g ammonium fluoride, 5 mL ultra pure water, 12 mL hydrogen peroxide and 12 mL concentrated nitric acid to polish the titanium plate; secondly, platinum plate was used as counter electrode and titanium plate as anode, then put it in 80 mL ethylene glycol solution containing 0.44 g NH4F and 8 ml H2O and then it was anodized at a constant potential of 20 V for 1 h; thirdly, wash the obtained materials with deionized water and calcine it in a muffle furnace at 450 °C for 2 h to get TiO2 nanotube array films, then take it out and place in a dust-free dryer for standby.

Preparation of FeS2/TiO2 nanocomposite films

FeS2/TiO2 nanocomposite films were prepared by hydrothermal deposition of FeS2 nanoparticles on TiO2 nanotubes. The detailed process is as follows: Firstly, FeCl3·9H2O was dissolved with secondary water in a 100 mL beaker, and prepare 35 mL FeCl3 solutions with concentrations of 5 mmol/L, 10 mmol/L and 20 mmol/L respectively, then dissolve thiourea ((NH2)2CS) with secondary water in another beaker to make Fe:S = 1:2, and then stir the two solutions for 30 min respectively and then set aside; Secondly, add 35 mL thiourea solution into FeCl3 solution and stir for 20 min after dropping to make FeCl3 and thiourea fully mixed; thirdly, transfer the mixed solution to a 100 mL Teflon reactor containing TiO2 nano film sheet, then placed it in the stainless steel jacket and put it into the blast drying oven, and set the heating temperature as 180 °C and heating time as 12 h; Finally, after the autoclave is cooled naturally, wash the obtained samples with deionized water and ethanol, and dried with dry cold air, then mark the obtained samples as 5-FST, 10-FST and 20-FST respectively for standby.

Characterization

The morphology of pure TiO2 and FeS2/TiO2 nanocomposite films were observed by scanning electron microscopy (SEM, Hitachi, S-8100); the chemical composition of FeS2/TiO2 nanocomposites was measured by X-ray photoelectron spectroscopy (XPS, PHI, Quantum 2000); and the crystal structures of TiO2 and FeS2/TiO2 composites were detected by X-ray diffraction (XRD, Japan Science and technology company, 5°/min); and the optical absorption properties of TiO2 and FeS2/TiO2 composites were characterized by uv-drs (Hitachi).

Photoelectrochemistry cathodic protection performance measurement

The photoelectrochemical properties are evaluated by measuring the photocurrent density time curve (I–t), and the test device is shown in Fig. 1a. The reference electrode and counter electrode of the electrochemical workstation CHI660E are short circuited, and a small resistance ammeter is formed between the working electrode and the grounding end. The electrolyte in the electrolytic cell is 0.1 mol/L Na2SO4, and the light source is the incident light filtered out of ultraviolet rays. As shown in Fig. 1b, the device for testing the performance of photoelectrochemical cathodic protection (including OCP, Tafel and EIS) is a dual cell system consisting of a corrosion cell containing 3.5 wt% NaCl solution and a photocell containing 0.1 mol/L Na2S solution, and the two cells are connected by Nafion membrane. The electrochemical work station (P4000 + ,USA) of three electrode system was used for electrochemical measurement: platinum plate as counter electrode, saturated calomel electrode as reference electrode, and copper wire as working electrode between 304SS electrode and optical electrode. The light source is a 300 W high pressure xenon lamp with visible light wavelength greater than 400 nm.

Figure 1
figure 1

(a) Photocurrent density measurement setup, (b) Experiment setup for electrochemical measurement.

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Results and discussion

Analysis of open circuit potential time curve

Figure 2 shows the open circuit potential time curves of 304SS electrode, 304SS electrode coupled with pure TiO2 nanotube array film, and 304SS electrode coupled with three kinds of FeS2/TiO2 nanocomposite films as photoanode under intermittent visible light and in 3.5 wt% NaCl electrolyte, and the OCP reflects the corrosion state of stainless steel electrode. It can be seen from the figure that the self corrosion potential of 304SS in 3.5 wt% NaCl corrosion medium is − 170 mV. As shown in curve (a), the electrode potential of 304SS coupling with pure TiO2 sample decreased from − 210 to − 340 mV under visible light, and the electrode potential after reaching stability was more negative than that of 304SS (− 170 mV), because TiO2 photo anode provided power supply for 304SS electrode under light condition, which reduced the electrode potential, thus realizing the effect of photoelectrochemical cathodic protection; when the light stopped, the OCP returned to the coupling electrode potential before the light, which indicated that pure TiO2 had no photoelectrochemical cathodic protection effect on 304SS electrode in the dark. Curves (b-d) show the OCP of 304SS coupling samples 5-FST, 10-FST and 20-FST as photoanodes, and the electrode potential of 304SS with three kinds of FeS2/TiO2 nanocomposite films decreased to − 455 mV, − 708 mV, − 361 mV under visible light, respectively, which indicates that the deposition of FeS2 nanoparticles on the surface of TiO2 nanofilms can improve the photoelectrochemical properties of TiO2. With the increase of reactant concentration in hydrothermal reaction, the photoinduced potential drop first increases and then decreases, and the photochemical cathodic protection ability also increases first and then decreases. Combined with the SEM surface morphology in Fig. 4, it is speculated that the reason may be that the excessive FeS2 nanoparticles not only reduce the active sites for light energy absorption of TiO2 films, but also increase the recombination sites of photoinduced electron hole pairs. When the light stopped, the electrode potential of 304SS coupled with three samples increased to − 320 mV, − 390 mV and − 310 mV, respectively, however, these three potentials are lower than that of 304SS bare electrode, which indicates that FeS2/TiO2 nanocomposite film still has good photoelectrochemistry cathodic protection effect under dark conditions, and the reason may be FeS2/TiO2 nanocomposite materials having certain energy storage function.

Figure 2
figure 2

OCP of (a) pure TiO2, (b) 5-FST, (c) 10-FST, (d) 20-FST.

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Analysis of photocurrent density time curve

Figure 3 shows the time curve of photocurrent density measured under intermittent visible light and 0.1 mol/L Na2SO4 solution by connecting TiO2 nanotube array film and FeS2/TiO2 composite film prepared at different concentrations as photoanode. The photocurrent density time curve can directly show the photoelectric conversion efficiency of photoelectric materials. The higher the photocurrent density, the higher the photoelectric conversion efficiency, and the stronger the metal protection. As shown in the figure, when the visible light irradiates the surface of the materials, the photocurrent provided by these materials as photoanodes to the cathode increases instantaneously and then stabilizes at a constant value, indicating that they all have photoelectric response performance. It can be seen from curve (a) that a very small photocurrent density (13 μA/cm2) is generated by the TiO2 photoanode, which is due to the large band gap of pure TiO2 and the small light absorption in the visible region. The curve (b-d) show that the current densities provided by the three kinds of FeS2/TiO2 composite films are 25 μA/cm2, 43 μA/cm2 and 18 μA/cm2, respectively, which are higher than those of pure TiO2 nano film as photoanode. The results show that the modification of TiO2 nano film by FeS2 nanoparticles greatly improves the photoelectric conversion efficiency, which is due to FeS2 semiconductor with narrow band gap is easy to absorb visible light, and the photo excited electrons migrate from the FeS2 conduction band to the TiO2 conduction band, while the photogenerated holes gather in FeS2, which realizes the separation of photogenerated electron–hole pairs, thus improving the light utilization and conversion efficiency of TiO227. Similar to pure TiO2 nanotube array film, many experiments on opening and closing light show that FeS2/TiO2 nanocomposite films have very high stability and can not be corroded by light.

Figure 3
figure 3

Photocurrent density time curve of TiO2 (a), 5-FST (b), 10-FST (c), 20-FST (d).

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Morphology characterization

The surface morphology of the samples is shown in Fig. 4, among them, Fig. 4a shows the SEM of pure TiO2, Fig. 4b–d shows the SEM of 5-FST, 10-FST and 20-FST, respectively. It can be seen from Fig. 4a that the tubular structure is formed by electrochemical oxidation, and these nanotubes whose diameter is 60–90 nm are closely arranged to form a thin film covering the smooth surface. The thickness of the tube wall is about 15–20 nm, and the length of the nanotube is about 450 nm (as shown in the cross-section at the upper right corner). Figure 4b is the SEM image of 5-FST sample, and it can be seen that nanoparticles with a diameter of 10–20 nm are attached to the edge of the tube mouth, and there is no deformation or collapse of TiO2 nanotubes after hydrothermal reaction, which indicates that the thermodynamic properties of TiO2 crystal are very stable. Figure 4c is the morphology of 10-FST sample, and it can be clearly observed that with the increase of FeS2 nanoparticles, the coverage area of FeS2 on the TiO2 nanotube film expands, and gradually agglomerates on the surface of TiO2 then fills the nanotubes, but the nozzle of TiO2 is still open. The morphology of 20-FST sample is shown in Fig. 4d, and the large FeS2 particles almost seal the mouth of TiO2 film. In conclusion, with the increase of the concentration of hydrothermal deposition reactants, the deposition amount of FeS2 nanoparticles increases, while the open part of TiO2 nanotubes decreases, as well as the contact area of photoelectrochemical reaction decreases, which indicates that the concentration of reactants will affect the morphology of FeS2/TiO2 nanocomposite films. Figure 3e is the energy spectrometer point distribution diagram of FeS2/TiO2 nanocomposite films. There is not only a large amount of Ti, O elements, but also a small amount of Fe and S elements were detected, and the ratio of Fe to s is about 1:2. For the analysis of the specific composition and the compound state of the substance, we will further determine it by means of X-ray photoelectron spectroscopy.

Figure 4
figure 4

SEM images of (a) pure TiO2, (b) 5-FST, (c) 10-FST, (d) 20-FST; (e) EDS of 10-FST.

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Crystal structure analysis of FeS2/TiO2 nanocomposite films

Figure 5 shows the XRD spectra of pure TiO2 nanotube array film sample, FeS2/TiO2 nanocomposite film sample and pure FeS2 powder prepared by hydrothermal method. As shown in the XRD curve of pure TiO2, there are two groups of characteristic diffraction peaks in the sample. A group of characteristic diffraction peaks with 2θ at 25.3°, 37.8°, 48.0°, 53.9° and 55.0° respectively belong to anatase TiO2 (JCPDF-21-1272), and these five diffraction peaks correspond to the 101, 004, 200, 105, 211 crystal face of TiO2, among them, 101 crystal face diffraction peak is the strongest, which indicates that 101 crystal face has the strongest activity; the 2 θ of the other group of characteristic diffraction peaks is 38.4°, 40.2°, 53.0°, 62.9°, 70.7° and 77.4° respectively, which is the characteristic diffraction peak of Ti metal lattice (JCPDF-44-1294), and the diffraction peak intensity of Ti is much stronger than that of TiO2, which verifies that the electrochemical oxidation of TiO2 is a nano material; while there is no diffraction peak of rutile TiO2 on the curve of this sample, which indicates that the crystal structure of calcined samples is anatase. In the XRD curves of FeS2/TiO2 nanocomposite film, in addition to the characteristic diffraction peaks of pure TiO2, there are also characteristic absorption peaks at 28.52° 33.05° 37.07° 40.75° 56.23° etc., which indicates that pyrite FeS2 nanoparticles were successfully deposited on anatase TiO2 nanofilms to form FeS2/TiO2 nanocomposites, which was consistent with the results of SEM. From the XRD spectra of FeS2 powder, it can be seen that the characteristic diffraction peak appears with 2θ at 28.51°, 33.04°, 37.07°, 40.76°, 47.42°, 50.49°, 56.27°, 59.01°, 61.68°, 64.28°, 76.59° and 78.96° respectively, and corresponding to (111), (200), (210), (211), (220), (311), (222), (023), (321), (331), and (420) of pyrite and crystal face (JCPDF-42-1340), respectively25, and there are no other impurity diffraction peaks in the curve, which indicates that the preparation method used in this study can prepare pyrite FeS2 nanoparticles with high purity and crystallinity.

Figure 5
figure 5

XRD patterns of pure TiO2, pure FeS2 and FeS2/TiO2 nanocomposites, the rhombus represents anatase type of TiO2 and star represents rutile type of TiO2.

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XPS analysis of FeS2/TiO2 nanocomposite films

In order to confirm the composition of the nanocomposite films more clearly, we used X-ray photoelectron spectroscopy to detect the valence orbital structure and valence of elements. Figure 6 shows the XPS spectra of FeS2/TiO2 nanocomposite film prepared under hydrothermal reaction time of 12 h, ferric chloride concentration of 0.15 mmol/L and reaction temperature of 180 °C, among them, Fig. 6a is the full spectrum scanning, and Fig. 6b–e is the high resolution narrow spectrum scanning map of elements. It can be seen from Fig. 6a that the characteristic orbital absorption peaks of Fe2p, O1s, Ti2p, S2p and C1s are detected in the sample, and there are no absorption peaks of other elements in the full spectrum, while the peak of C1s is the impurity peak when the instrument is calibrated. Figure 6b is a high resolution narrow spectrum of Fe2p, and it can be seen that the binding energies at 707.1 eV and 719.4 eV correspond to the orbits of Fe2p3/2 and Fe2p1/2, and the distance between the two peaks is 12 eV, which is similar to that of FeS2. Figure 6c is a high-resolution narrow spectrum of S2p orbit, and 163.8 eV corresponds to the characteristic peak of binding energy of S2p orbit. According to the literature, the S element in the sample is − 1 valence, so FeS2 exists in the complex28. Figure 6d is a high resolution narrow-band XPS image of Ti2p, and the binding energies of the two characteristic absorption peaks are 458.4 eV and 464.2 eV, respectively, which are corresponding to the orbital absorption peaks of Ti2p3/2 and Ti2p1/2, indicating that the valence state of Ti is + 4, and the Ti element in the sample mainly exists in the form of TiO2. Figure 6e is a high resolution narrow spectrum of O1s, and it can be seen from the figure that the characteristic peak of binding energy at 529.9 eV corresponds to the metal oxide, which is consistent with the narrow spectrum scanning of Ti2p, and due to the O1s peak is very sharp, there is no other oxide in the sample. In conclusion, the composition of the nanocomposite is only FeS2 and TiO2, which is consistent with the results of EDS and XRD.

Figure 6
figure 6

XPS survey spectra (a), Fe2p (b), S2p (c), Ti2p (d), O1s (e) core level spectrum of FeS2/TiO2.

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Optical absorption properties of FeS2/TiO2 nanocomposite films

Figure 7 shows the UV–Vis diffuse reflectance spectra of pure TiO2 nanotube film, pure FeS2 powder tablet and FeS2/TiO2 nanocomposite film. It can be seen from the curve of pure TiO2 sample that the light absorption edge of pure TiO2 nano film is 387 nm, and the light absorption intensity in visible light region is very weak, corresponding to the energy band width of TiO2 is 3.2 eV. From the curve of pure FeS2 sample we can see that the light absorption edge of pyrite FeS2 is 780 nm, and the radiation in visible spectrum has strong light response, and the corresponding band gap is 1.5 eV, indicating that pyrite FeS2 is an excellent semiconductor material with narrow band gap. According to the curve of FeS2/TiO2 nanocomposite films, the light absorption edge of FeS2/TiO2 nanocomposite is 496 nm, and the corresponding band gap is 2.5 eV, which indicates that the deposition of FeS2 nanoparticles on the TiO2 nano film can expand the light absorption range to the visible light region, and reduce the band gap of TiO2. In summary, nanosized pyrite FeS2 has a very significant effect on improving the optical absorption properties of TiO2 nanotube films.

Figure 7
figure 7

UV–vis diffraction reflectance spectra of the pure TiO2, pure FeS2 and FeS2/TiO2.

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Tafel polarization curve analysis of FeS2/TiO2 nanocomposite films

After the metal contacts with the medium in the environment, there are multiple electrode reactions on the metal surface. The anodic reaction makes the metal dissolve and enter the solution in the form of ions, which is called anode process; and the cathodic reaction is that the medium on the metal surface absorbs the electrons from the anode, and the metal does not dissolve. The existing state of metal depends on the addition of total cathodic reaction and total anode reaction, and the anode process causes electrochemical corrosion of metal, while the principle of cathodic protection is the polarization of metal under external conditions, therefore, the total potential of metal changes from corrosion potential to negative, the total cathodic current increases and the anode current decreases. Figure 8 shows the Tafel potentiodynamic polarization curve of 304SS electrode coupled with TiO2 nanotube array film and FeS2/TiO2 nanocomposite film photoanode under visible light condition, and the corrosion medium is 3.5 wt% NaCl solution. As shown in curve (a), the corrosion potential of 304SS bare electrode is − 180 mV in 3.5 wt% NaCl solution. It can be seen from the curves (b) and (c), under visible light irradiation, the potential of 304SS coupled with pure TiO2 and FeS2/TiO2 photoanode shifted negatively to − 490 mV and − 740 mV, separately, and the 304SS was in cathodic protection state. It can also be seen from the figure that the current on the surface of 304SS electrode coupled with pure TiO2 and FeS2 photoanode is larger than that of bare 304SS electrode, which indicates that the photoanode provides electrons for 304SS under visible light, and this result is consistent with the open circuit potential time curve and photocurrent density time curve. According to the principle of cathodic protection, the electrode potential of metal decreases, the current increases, and the electrode reaction of metal corrosion is inhibited, which shows that both pure TiO2 and FeS2/TiO2 can provide photoelectrochemical cathodic protection for 304SS under visible light. Compared with pure TiO2, FeS2/TiO2 has better cathodic protection effect on 304SS, which indicates that FeS2 modified TiO2 improves the photoelectrochemical cathodic protection performance of TiO2 nanotube array film.

Figure 8
figure 8

Tafel polarization curves of bare 304SS electrode (a), and 304SS coupled with pure TiO2 (b) and FeS2/TiO2 (c) under visible light illumination.

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EIS analysis of FeS2/TiO2 nanocomposite films

EIS can provide valuable electrochemical information of metal/solution interface, so it is used to evaluable the effect of photochemical cathodic protection on the prepared films29. Figure 9a shows the Nyquist diagram of 304SS in 3.5 wt% NaCl solution without coupling and coupling FeS2/TiO2 nano film photoanode, and each curve has only one capacitance arc. Obviously, under visible light irradiation, the capacitance arc of 304SS coupling FeS2/TiO2 nano film photoanode is much smaller than that of 304SS bare electrode, and the difference between them is two orders of magnitude. The EIS spectrum can be simulated by the equivalent circuit shown in Fig. 9b. In the equivalent circuit model, RS, RCT and CPE represent solution resistance, charge transfer resistance and constant phase element respectively, and the main purpose of EIS measurement is to obtain the RCT value of coupled 304SS in corrosion cell to compare the electron transfer rate under light and dark conditions. When 304SS was coupled with thin film photoanode under light, photogenerated electrons were transferred from photoanode to steel to participate in electrochemical reaction, which accelerated the cathodic reaction of 304SS stainless steel/solution interface, showed low RCT value, and 304SS cathode polarization reduced corrosion. Therefore, FeS2/TiO2 nanocomposite films can provide excellent photochemical cathodic protection performance.

Figure 9
figure 9

(a) Nyquist plots of 304SS, 304SS coupled with FeS2/TiO2 under visible light illumination and dark state conditions ; (b)The equivalent circuit model of FeS2/TiO2 photoanode under illumination.

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Mechanism analysis of photoelectrochemical cathodic protection

The electron transfer process of FeS2/TiO2 nanocomposite film coupled with 304SS electrode under visible light is shown in Fig. 10. It takes less photon energy to excite FeS2, and the electron in the valence band of FeS2 can be excited by visible light and then transited to the conduction band. Because the conduction band potential of FeS2 is lower than that of TiO2, the conduction band electrons in FeS2 can be transferred to the conduction band of TiO2, while the holes in FeS2 remain in the valence band, which greatly improves the separation efficiency of photogenerated electron–hole pairs. Under the action of external circuit, photogenerated electrons are transferred to 304SS and gathered on the surface of it, which makes 304SS cathode polarized to achieve the purpose of cathodic protection. Therefore, FeS2/TiO2 nanocomposite film has excellent photoelectrochemical cathodic protection effect on 304SS under visible light irradiation.

Figure 10
figure 10

The mechanism schematic diagram of the photoelectochemical cathodic protection.

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Conclusion

  1. (1)

    FeS2/TiO2 nanocomposite films were successfully prepared by anodic oxidation and hydrothermal methods, and when the concentration of reactants was designed to be 10 mmol/L, FeS2/TiO2 nanocomposite films had the optimal surface morphology of absorbing sunlight.

  2. (2)

    After the modification of FeS2 nanoparticles, the light absorption range of TiO2 extends from UV to visible, which not only improves the separation efficiency of photogenerated electron–hole pairs, but also increases the photoelectric conversion ability.

  3. (3)

    Compared with pure TiO2, the modification of FeS2 nanoparticles on the surface of TiO2 nanotube array film greatly improves the photoelectrochemistry cathodic protection performance of 304SS.

  4. (4)

    Under visible light irradiation, the OCP of 304SS coupled with the composite can be reduced to about − 700 mV, and the electrode potential of the stainless steel can still be maintained at − 400 mV after the light is turned off, that is, FeS2/TiO2 Nanocomposite filmscan still play the role of electrochemical cathodic protection in the dark.