Ranjith
Bose
*ab,
Surya Prakash
Gajagouni
c,
Imad
Barsoum
c,
Sung Oh
Cho
d and
Akram
Alfantazi
*ab
aDepartment of Chemical and Petroleum Engineering, Khalifa University, Abu Dhabi 127788, United Arab Emirates. E-mail: ranjith.bose@ku.ac.ae; akram.alfantazi@ku.ac.ae
bEmirates Nuclear Technology Center (ENTC), Khalifa University, Abu Dhabi 127788, United Arab Emirates
cDepartment of Mechanical and Nuclear Engineering, Khalifa University, Abu Dhabi 127788, United Arab Emirates
dDepartment of Nuclear and Quantum Engineering, Korea Advanced Institute of Science and Technology (KAIST), Daejeon 34141, South Korea
First published on 26th July 2024
Stainless steel (SS)-based electrocatalysts have attracted considerable attention in renewable energy research, emerging as viable replacements for precious noble metal-based catalysts owing to their cost-effectiveness and widespread availability. Further, SS's ability to function as an electrode material in alkaline water electrolyzers and its inherent corrosion resistance make it a key component of sustainable energy solutions. This study focuses on the fabrication of a self-ordered nanoporous oxide layer on SS through an anodization method, followed by an investigation into the electrocatalytic activity of the resulting films for hydrogen evolution reaction (HER) and corrosion properties. Anodization creates a highly organized nano-porous metal oxide structure featuring extensive surface areas that offer abundant active sites for electrochemical reactions via the oxide formation-dissolution mechanism. The nano-porous oxide film produced demonstrates exceptional HER activity, reaching a cathodic current density of 10 mA cm−2 with a minimal overpotential of 343 mV (versus the reversible hydrogen electrode (RHE)) in a strong alkaline medium. Moreover, the stability of the derived nano-porous oxide film remains unaffected during 50 hours of uninterrupted electrolysis, demonstrating remarkable operational resilience. Conversely, potentiodynamic polarization measurements reveal that the resulting films exhibit superior corrosion resistance in both NaCl and KOH electrolytes compared to bare SS. This enhanced resistance is attributed to the self-ordered nano-porous structure, which fosters the construction of a more uniform film with a more robust passive layer. The straightforwardness of the procedure and the widespread availability of the initial material make this an unexpectedly effective endeavour. The research demonstrated that anodized SS can achieve both corrosion resistance and catalytic activity for the HER, making this material system a viable candidate for alkaline water electrolyzer systems.
Stainless steel (SS) has long been celebrated for its remarkable combination of mechanical strength, durability, and resistance to corrosion and also is a crucial material in alkaline water electrolyzers due to its cost-effectiveness, durability, and electrocatalytic properties.17–20 This alloy, primarily composed of iron (Fe), chromium (Cr), and other alloying elements, creates a passive oxide layer over the surface, which acts as a protective barrier against corrosive environments.18,21 However, despite its inherent corrosion resistance, SS can still be susceptible to certain aggressive conditions, particularly in applications where it is exposed to harsh chemical environments or high temperatures. To nullify this effect and further improve the performance of SS in demanding applications, researchers have turned to surface modification techniques such as anodization.21–25 Anodization involves the controlled electrochemical oxidation of the metal surface, leading to the formation of a thick and dense oxide layer with tailored properties. This process enhances the material's resistance to corrosion and introduces new functionalities, such as improved catalytic activity for electrochemical reactions.24–27 There has been growing interest in the anodization of SS for applications beyond traditional corrosion protection in recent years. One area of particular interest is the development of anodized SS electrodes with enhanced catalytic activity toward the electrochemical water splitting reactions in alkaline solutions, making it a practical choice for these electrolyzers.17,21–23,25 Despite recent advancements, there's still room for improvement in enhancing the HER activity, particularly in optimizing the anodization process and advancing binder-free electrodes. The anodization process typically involves an oxide layer formation on the SS surface, which can introduce surface defects like vacancies, dislocations, or edge sites.25,26,28 These defects can significantly influence electrocatalytic activity and the corrosion resistance properties of the material. Conversely, traditional electrodes often rely on binders to immobilize catalyst particles, which can hinder mass transport and create additional resistance, thereby limiting HER kinetics. However, binder-free electrodes offer a solution to these challenges by enabling direct contact between the catalyst and electrolyte, thus improving mass transport and enhancing electrochemical activity.29,30
By considering the importance of these key properties of SS and their interplay in water electrolysis systems, we develop a self-organized nano-porous oxide film on the surface of SS by an electrochemical anodization strategy using an ammonium fluoride and ethylene glycol-based solution. With this straightforward approach, SS surface morphology, chemical states, and electrochemical properties are tailored to create an electrochemically active nano-porous oxide film. This enhanced surface architecture facilitates the water molecules' adsorption and dissociation properties, thereby accelerating the kinetics of the HER and increasing the overall efficiency of electrochemical hydrogen production. Furthermore, the anodized oxide layer provides an additional barrier against corrosion, protecting the underlying SS substrate from degradation during prolonged electrochemical operation. This enhanced corrosion resistance is significant in alkaline electrolytes, where the HER typically occurs, as it ensures the long-term stability and durability of the electrode material.
A comprehensive theoretical hypothesis is presented in eqn (1)–(4) to understand the creation of oxide species from SS substrate. In first step, anodic oxidation occurs at SS, generating metal cations and electrons.24,31–33 Subsequently, in the second step, the ammonium fluoride in the electrolyte solution reacts with the metal cations (Mn+) to produce soluble metal fluoride complexes. These complexes aid in the dissolution of intermediate oxide layers formed during anodization, as observed in the third step. Meanwhile, in the fourth step, the applied voltage promotes the development of a dense and thick anodic oxide layer on the SS surface through electrochemical oxidation. In addition, gas evolution, specifically the release of hydrogen gas during anodization, leads to the creation of pores within the anodic oxide layer.34,35
M → Mn+ + ne− | (1) |
Mn+ + xNH4F → MFx + xNH4+ | (2) |
MO + xNH4F → MFx + H2O + xNH4+ | (3) |
MFx + yH2O → MxOy + zHF | (4) |
Moreover, Fluoride ions play two crucial roles in the oxide formation process. Firstly, they generate water-soluble [MFx]y− ions, which effectively hinder the formation of hydroxides.24,31,36 Secondly, they aid in the erosion of existing metal oxides, leading to the formation of a nanotubular layer rather than a dense one. Due to their ability to initiate chemical dissolution reactions and small ionic size, a small fraction of fluoride ions can be incorporated into the metal oxides.31,37,38 Upon annealing in air, fluoride ions are liberated from the metal oxide film surface as hydrogen fluoride (HF).38,39
In addition, the voltage applied during anodic oxidation was significantly influenced by the formation of self-organized nanopore arrays, indicative of the consistency of pores on SS surfaces. Utilizing the observed influence, anodization was performed on SS samples at various operating voltages-specifically, 65, 75, and 85 V- for a duration of 30 minutes in an ethylene glycol electrolyte solution containing 0.1 mol per dm3 NH4F and 0.1 mol per dm3 H2O. The impact of varying anodization voltages on SS was assessed by analyzing surface morphology using scanning electron microscope (SEM) imaging. Fig. 1 displays the anodized SS's top surface, while Fig. S2† presents digital pictures depicting the films' macroscopic appearance. Moreover, SEM images provide comprehensive insights into the surface morphological characteristics. SEM imaging also confirmed the existence of self-organized nanopore arrays in all samples of anodized SS substrates. In addition, the SEM images display notable differences in the regularity of pores on the anodized SS films under an applied voltage of 75 V, contrasting with those untreated and anodized SS at 65, and 85 V (Fig. S3 and S5†). The SEM image of the sample's surface anodized at 75 V reveals a well-organized nanoporous oxide layer with a diameter ranging from 120 to 180 nm. However, the regularity of these highly ordered pores is notably disrupted by a further increase in voltage to 85 V (Fig. S5 and S6†). The voltage significantly affects the size and regularity of pores over the stainless steel's surface, which is concurrent with the literature.32,40 Previous investigations have proved that nanoporous arrays, including anodic aluminum oxide (AAO) and FeCrAl self-organizing porous structures, exhibit perfect self-ordered pore formations only when the potential does not exceed its breakdown threshold.32,41 Also, it can be observed that the interhole distance of the anodic porous oxide obtained during anodization depends on the anodization voltage, indicating a voltage-dependent formation of the nanohole arrays. The cross-sectional SEM image (Fig. 1D–F) authorized the presence of a nanoporous oxide layer comprising an ordered array of uniformly sized holes over the stainless steel's surface under the 75 V condition, exhibiting a curved and branched structure. Conversely, under the conditions of 65 V and 85 V, the cross-sectional SEM image revealed a disordered structure (Fig. S5†), indicating a significant influence of voltage on the formation of nanoporous arrays on the surface of SS. Based on the observed formation process of the ordered structure described above, it can be inferred that the anodic oxidation conducted in ethylene glycol-based electrolyte aligns more closely with the flow model proposed by Skeldon et al.42,43 In Fig. 1G and H, an HR-TEM image of the SS-75 V sample reveals distinct lattice fringes, with a lattice spacing of 0.267 nm corresponding to the (104) plane of the hematite phase, consistent with the previously reported work.24Fig. 1I displays the EDX spectra of the anodized SS sample at 75 V, while the inset of Fig. 1I illustrates the weight percentage of each element, accompanied by the corresponding EDX spectrum. The surfaces of the samples exhibit a significant enrichment in chromium (Cr) species and a considerable increase in oxygen (O) species following surface anodization compared to the bare SS (Fig. S4†). This augmentation of Cr and O species post-anodization aligns well with previous findings, indicating that the metal-oxide constitutes a major component of the nanoporous oxide layer.18,21,23,24 Furthermore, the well-ordered nano-array structures, resembling honeycomb-like patterns, possess high surface areas, and these structures would have been beneficial to improve the surface-anodized SS catalytic activity towards the HER and the bottom on the barrier layer (Cr-rich oxide layer; Fig. S7†) may impede the penetration of corrosive ions to the SS's surface atoms.
Fig. 2A presents XRD results of both bare (untreated) SS and anodized SS samples. In all cases, three prominent peaks are observed at 43.85° (111), 51.06° (200), and 74.93° (220), which correspond to the austenite SS peaks (dot circle) originating from the SS304 substrate. These findings align well with previous studies and are consistent with the JCPDS reference card number 33-3097. Notably, the anodized samples (SS-65 V, SS-75 V, and SS-85 V) exhibited the presence of some low-intensity peaks with significant counts within the diffraction angle range of 20° to 40° (Fig. S8†). These peaks correspond to the Fe2O3 (hematite) phase of iron oxide (asterisk, JCPDS 33-0664). The XRD analysis reveals notable resemblances among the anodized samples, suggesting the absence of any crystallographic changes during the anodization process, regardless of the applied voltage variations. The consistent diffraction pattern observed across various anodized samples may be attributed to the relatively thin thickness of the nano-porous oxide film developed on the surface of SS. These thin films are challenging to detect using XRD due to its inherent limitation as a bulk characterization technique. Fig. 2B presents the Raman spectra obtained from the anodized SS samples, which were utilized to identify the chemical states of the samples. The spectra exhibit similarity and are characteristic of the α-Fe2O3 (hematite) phase, displaying peaks at approximately 228, 293, 416, 674, and 1331 cm−1. These observed peaks align closely with previously reported Raman data for the hematite phase.25,44–47 The peak at 228 cm−1 is attributed to the A1g mode, while those around 293 cm−1 and 416 cm−1 are assigned to the Eg modes. Additionally, the peak at approximately 674 cm−1 is linked to disorder effects and the existence of Fe2O3 nanocrystals, while the peak at around 1331 cm−1 is associated with hematite two-magnon scattering. It was further noted that the Raman spectrum of the anodized SS under voltages of 75 V and 85 V exhibits peaks characteristic of a magnetite (Fe3O4) phase, notably a strong band at 691 cm−1, alongside hematite peaks.25,44,47 This suggests that both samples contain a mixture of two phases. Specifically, in the case of 75 V anodization, the magnetite phase's composition appears slightly higher than the sample anodized at 85 V, as evidenced by the peak broadening in the respective Raman spectra. The coexistence of hematite and magnetite phases in the anodized SS sample may be attributed to the complex oxidation processes and the specific electrochemical conditions involved during the anodization process.48,49 The crystallographic structure and surface morphology of these iron oxide phases could be crucial in evaluating the electrocatalytic activity of the anodized SS towards the HER. Specific crystal facets and defects in these phases can promote hydrogen intermediate adsorption and enhance the overall catalytic efficiency.18,20
Fig. 2 Structural and spectroscopic characterization of the anodized SS nano-porous oxide layer. (A) X-ray diffractograms from the films. Identified phases are represented by symbols (dot circle: austenite SS peaks originating from the SS304 substrate; asterisk: hematite phase of iron oxide-Fe2O3). (B) Raman spectra of the anodized SS samples. The observed peaks are consistent with previously reported Raman data for hematite and magnetite phases.39,40 (C–F) XPS characterization of sample SS-75 V. (C) Fe 2p core levels – it shows Fe2+ and Fe3+ oxidation state. (D) Ni 2p core levels – Ni2+ oxidation state suggests NiO formation. (E) Cr 2p core levels – Cr is present in the form of CrIII. (F) O 1s core levels – this indicates mixed oxide states are present. a.u., arbitrary unit. |
XPS was employed to conduct further investigations into the as-prepared material's surface chemical states and material constituents. The survey spectra (Fig. S9†) distinctly specified the existence of iron (Fe), nickel (Ni), chromium (Cr), and oxygen (O), implying the formation of nano-porous oxide thin films on the surface of the anodized SS. In the high-resolution Fe 2p spectrum of the SS-75 V anodized sample (Fig. 2C), peaks at 709.8 and 711.7 eV were observed, corresponding to Fe2+ and Fe3+.18,21,22,30 This observation suggests the coexistence of magnetite and hematite phases in SS-75 V, consistent with the findings from the Raman spectra. This confirmation indicates a reduction in the net oxidation state of Fe as the phase transition takes place, leading to the creation of oxygen vacancies. It is widely recognized that materials with self-doped oxygen vacancies, owing to the presence of vacant sites facilitating the transport of electrons or ions, may exhibit enhanced electron or ion conductivity compared to fully oxidized metal oxides.25 The presence of two peaks observed at 854.8 eV (2p3/2) and 873.2 eV (2p1/2) in the Ni 2p spectra (Fig. 2D) indicates the formation of NiO (Ni2+ oxidation state).21,24,50Fig. 2E shows a deconvolution of Cr 2p spectrum. In the surface-oxidized SS, Cr has undergone oxidation to a higher oxidation state, with the presence of Cr3+ (Cr2O3-576.4 eV; Cr(OH)3-577.8 eV) evident in the SS-75 V sample. This presence could manifest in the form of Cr2O3, Cr(III) hydroxide, or a combination of both forms.18,21,23,33 The O 1s spectra (Fig. 2F) exhibited two characteristic peaks at 530.4 eV and 531.8 eV, indicating the existence of passive metal oxides with mixed oxidation states on the surfaces of the anodized SS samples.22,24 The thorough and comparative XPS analysis has conclusively demonstrated the oxidation of crucial elements within SS, along with the notable observation of both iron oxide phases present on the surface of SS-75 V. Additionally, a pronounced presence of Ni2+ with FeCr oxides significantly influences the electrochemical behavior.
M + H2O + e− = M–Hads + OH− | (5) |
M–Hads + H2O + e− = M + H2 + OH− | (6) |
2M–Hads = 2M + H2 | (7) |
The Volmer step (5) involves breaking a water molecule and the adsorption of hydrogen onto a vacant site of the electrode/catalyst surface. Subsequently, hydrogen production occurs through either an electrochemical process (Heyrovsky step (6)) or a chemical process (Tafel step (7)). Several studies have indicated that, at low overpotentials, the HER mechanism entails the Volmer step followed by concurrent Heyrovsky and Tafel steps, while at higher overpotentials, the Tafel step becomes insignificant, and the reaction primarily follows the Volmer–Heyrovsky mechanism. In practical applications, a smaller Tafel slope leads to an enhanced HER rate with a steady increase in overpotential, thereby offering advantageous outcomes.
The EIS spectra were conducted during the HER activity to study the electrode kinetics (Fig. 4F). Additionally, a tedious R–C equivalent diagram was employed to analyse the kinetic disparities among these electrodes, as depicted in the inset of Fig. 4F. The smaller-semicircle observed in the low-frequency region of the Nyquist plot indicates a heightened HER process, correlating with reduced charge transfer resistance (Rct). Specifically, the charge-transfer resistance (Rct) observed for the SS-75 V electrode was notably lower compared to that of the SS-65 V and SS-85 V electrodes, suggesting a significantly enhanced electron transport capability for the hydrogen evolution reaction (HER) in the SS-75 V electrode. This trend aligns with the findings from the Tafel slopes and polarization curves. The robust stability and elevated HER activity of the developed binder-free electrode of SS-75 V, facilitated by the synergistic intervention of nanoporous oxide structure and active sites, may be assumed to occur by the following factors. The electrochemical active surface area (ESCA) of the anodized SS samples was estimated using the double-layer capacitance (Cdl) obtained from cyclic voltammetry (CV) curves. CV curves of the prepared electrodes at various scan rates in the 0.88–1.12 V vs. RHE are presented in Fig. S11.† The calculated Cdl values (Fig. 3G) were 0.00082, 0.00165, and 0.00124 μF cm−2 for SS-65 V, SS-75 V, and SS-85 V samples, respectively. Notably, SS-75 V demonstrated a significantly larger double-layer capacitance compared to the other two samples. This indicates that SS-75 V can expose more effective active sites due to its proportional relationship with surface area and material conductivity, thereby contributing to enhanced HER activity.
Further analysis of the SS-75 V sample was conducted using SEM, Raman, and XPS to determine any potential alterations to the valence state over the surface, phase change, and microstructure change after 50 hours of CA operation. Fig. 4A illustrates that the surface (nano-porous) morphology of the SS-75 V electrode remains unchanged even after continuous 50 h CA studies. Raman spectra (Fig. 4B) showed attenuation and broadening of peaks corresponding to the hematite and magnetite phases with the progression of the long-term stability test, and also, the Raman spectra data matched with the previously reported Raman data of Fe0.993+O(OH).44 This undoubtedly indicates that the crystallinity of the oxide layer decreased as metal hydroxide formed, which has a higher electrocatalytic activity.25,56 The Fe 2p, Ni 2p, and Cr 2p XPS spectra (Fig. 4C–E and S12†) were examined, with their corresponding peaks interpreted from Fig. 4C (Fe3+: 711.2 eV), Fig. 4D (Ni(OH)2: 855.4 eV), and Fig. 4E (Cr2O3: 576.3 eV; Cr(OH)3:577.7 eV). These findings align with the characterization work on anodized SS samples previously reported by Kim et al.25Fig. 4F displays the O 1s spectrum, highlighting all component peaks and their respective contributions. The prominent band observed at a binding energy of 530.1 eV is because of the oxygen contribution from oxide ions (M–O), while the band at 531.6 eV is associated with oxygen from hydroxide (M–(OH)2).57,58 Additionally, the peaks at 532.9 eV are linked to water's physicochemical absorption.57,58 Together, these peaks indicate the construction of hydroxyls (OH−) and lattice oxygen (O2−) over the SS-75 V surface. Based on these findings, it is plausible to deduce that the formation of metal hydroxides and the preservation of highly organized nano-porous transition metal oxide structures with extensive surface areas occur. This facilitates the creation of multiple active sites for electrochemical reactions, which progressively multiply as cathodic current is applied for hydrogen evolution, resulting in the self-activation of the electrode and a gradual reduction in overpotential for HER.
Fig. 5 Corrosion testing of anodized SS electrodes. (A and B) Potentiodynamic polarization curves for bare and anodized SS corrosion testing in (A) 3.5% NaCl and (B) 1 M KOH solution. |
Parameter | NaCl | KOH | ||||||
---|---|---|---|---|---|---|---|---|
Bare SS | SS-65 V | SS-75 V | SS-85 V | Bare SS | SS-65 V | SS-75 V | SS-85 V | |
E corr; (mV) | −66.80 | −15.50 | −58.50 | 69.6 | −212.0 | −179.0 | −343.0 | −212.0 |
I corr; (μA) | 16.10 | 12.90 | 0.915 | 4.930 | 139.0 | 65.70 | 6.680 | 102.0 |
β a; (V per decade) | 104.2 × 10−3 | 82.40 × 10−3 | 311.1 × 10−3 | 486.0 × 10−3 | 1.233 | 987.6 × 10−3 | 97.90 × 10−3 | 2.052 |
β c (V per decade) | 205.6 × 10−3 | 172.5 × 10−3 | 228.1 × 10−3 | 395.5 × 10−3 | 1.568 | 457.5 × 10−3 | 125.1 × 10−3 | 552.5 × 10−3 |
C R (mpy) | 7.383 | 5.908 | 0.599 | 2.256 | 4.623 | 2.182 | 0.221 | 3.370 |
Footnote |
† Electronic supplementary information (ESI) available: Details of materials characterization, electrochemical experiments, digital images of the experimental setup, XRD and Raman data, SEM images of bare SS and anodized SS at 65, 85 and 90 V samples, and XPS survey spectrum of anodized samples. See DOI: https://doi.org/10.1039/d4ta03317e |
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