Open Access Article
Kayalvizhi Rajagopal and
Abirami Natarajan
*
Department of Chemistry, College of Engineering and Technology, SRM Institute of Science and Technology, Kattankulathur, Tamil Nadu-603203, India. E-mail: abiramin@srmist.edu.in; Tel: +91 9941223928
First published on 7th April 2026
Developing low-cost, highly active electrocatalysts for electrochemical water splitting is crucial for decreasing the demand for energy in the future. Water splitting has been addressed as a feasible option for storing electrical energy. Researchers are interested in designing non-toxic, high-performance, and cost-effective catalysts for the oxygen evolution reaction (OER) and the hydrogen evolution reaction (HER). Herein, spherical structured Ti0.5Sr0.5O3 catalysts, which are materials made from titanium and strontium oxides, are produced using a simple solid-state technique. XRD, Raman, FE-SEM, TEM, XPS, and FT-IR spectroscopy were performed to confirm the crystal structure, morphology, and element composition of the Ti0.5Sr0.5O3. In alkaline electrolyte 1.0 M KOH solution, Ti0.5Sr0.5O3/NF has good OER activity, with an overpotential and a Tafel slope of 299 mV and 152.5 mV dec−1, respectively. It also exhibits strong HER activity, with overpotential and a Tafel slope of 101.6 mV and 179 mV dec−1, respectively. The present research employs an innovative development approach for a low-cost, highly efficient water-splitting catalyst that aligns with the United Nations' Sustainable Development Goal 7 for affordable and clean energy.
It is imperative to develop sustainable energy sources as alternatives to address the energy crisis and its associated environmental problems. Researchers have extensively studied a number of renewable energy sources, including wind, solar, biopower, and hydropower, as potential sustainable alternatives to fossil fuels. As a result, there is an urgent need to create new methods for converting, storing, and utilizing the electrical energy created.3 Hydrogen, an energy carrier, can efficiently transform electrical energy into chemical energy (hydrogen fuel) using water electrolysis.4 This is an intriguing method for meeting the goal of energy conversion and storage. Furthermore, hydrogen has a high gravimetric energy density and produces ecologically favourable combustion products, making it a viable alternative to conventional fossil fuels.5 On the other hand, hydrogen is produced through natural gas reforming and coal and oil gasification, all of which require the usage of fossil fuels and emit CO2.6 To this aim, water splitting appears as an interesting technique for hydrogen production because it is both ecologically friendly and sustainable, in addition to creating high-quality hydrogen (more than 99.9%).7 Several factors influence the total efficiency of hydrogen fuel generation, and these are the primary driving forces behind full water electrolysis. Increasing the overall reaction rate creates an external bias of ≤1.23 V against RHE, which exceeds the theoretical value.8 The OER's four-proton-linked electron (4e−) transport mechanism may explain the observed behavior.9 Additionally, a three-electrode electrolyzer that is incorporated within a bigger device demonstrates a high conversion efficiency while operating at 1.8–2.0 V. This additional voltage input creates a significant difference between the electrocatalyst's cost and its electrochemical performance. As a consequence, to speed up both half-reactions, it is necessary to have a wide surface area, high stability, a large number of active sites, and consistent adsorption of effective electrocatalysts.10 While noble-metal catalysts such as Pt, IrO2, and RuO2 exhibit excellent performance, their high cost and limited availability hinder large-scale application.11
Transition-metal oxides, particularly perovskite-type oxides, have attracted attention as cost-effective alternatives due to their structural versatility, tunable electronic properties, and stability under electrochemical conditions.12 Transition metal oxides have been shown in both theoretical and practical studies to offer significant potential for water electrolysis.13 In this context, spherical Ti0.5Sr0.5O3 offers potential as a bifunctional catalyst, combining favorable electronic structure and surface properties for both OER and HER, while utilizing abundant and inexpensive elements. Despite some studies on Ti0.5Sr0.5O3 synthesis and characterization, its bifunctional catalytic performance, mechanistic understanding, and structure–activity relationships remain largely unexplored. Titanium and strontium have received a lot of attention in the field of electrocatalysis compared to other metals, due to their low electronegativity, small particle size, form, strong electrical capacity, increased number of active sites, and wide surface area.14 Furthermore, the increasing interaction between strontium and titanium enhances superconductivity and chemical stability, suggesting an effective OER/HER reaction pathway. To manufacture the composite catalyst, we took a conventional, solid-state technique. Therefore, this work investigates Ti0.5Sr0.5O3 as a bifunctional electrocatalyst for water splitting, focusing on its synthesis, structural and electronic properties, and electrochemical performance, which reveal its potential as an efficient and sustainable material for hydrogen production. In accordance with the findings of X-ray diffraction, the heterojunction approach is responsible for modifying not only the electrical structure but also the phase formation of bifunctional catalysts. HR-TEM analysis was also utilized in order to evaluate the spherical form of the synthetic composite as well as the quality of its material. In a 1.0 M KOH solution, Ti0.5Sr0.5O3/NF has good OER activity, with an overpotential of 299 mV and a Tafel slope of 152.5 mV dec−1. It also exhibits strong HER activity, with an overpotential of 101.6 mV and a Tafel slope of 179 mV dec−1. Both the ECSA and EIS evaluations revealed that this diverse structure had efficient transportation pathways. These channels are created by increasing the contact area of the two materials and lowering the energy barriers. The LSV approach was also used to analyze the electrochemical behavior of Ti0.5Sr0.5O3/NF on a three-electrode setup. Furthermore, the Ti0.5Sr0.5O3/NF remained durable up to 40 hours. The utilization of transition metals provides a novel approach to the study and design of diverse bifunctional electrocatalysts. This approach has the potential to significantly enhance the bifunctional electrochemical water splitting on a wide scale.
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| Fig. 2 (a–d) FESEM images; (e and f) TEM images; (g) lattice spacing; (h) selected area electron diffraction pattern; (i–l) elemental mapping of Ti0.5Sr0.5O3. | ||
m phase P4332 phase. These predict that Ti0.5Sr0.5O3 will have sharp, well-defined peaks indicate good crystallinity, which may influence electronic conductivity and stability. FT-IR spectral studies were utilized to evaluate the chemical composition of the as-prepared Ti0.5Sr0.5O3 as well as the surface functional groups, as shown in Fig. 1b, demonstrating a band at 662.8 and 756.7 cm−1, indicating Ti–O–Ti stretching vibrations.17 Sharp bands at 819.8 and 872.5 cm−1 indicate Sr stretching and Sr–O vibrations, respectively. All of these peaks indicate the presence of Ti and Sr in the Ti0.5Sr0.5O3 sample. Peaks at 1030.4 cm−1 correspond to TiO2, 1093.8 and 3406.7 cm−1 for titanium, 1661.6 cm−1 for Ti–OH, 1293.3 cm−1 for CO stretching, and 1556.4 cm−1 for asymmetric stretching COO− vibrations.18 Raman spectroscopy was used to study the product structure based on lattice vibrations, showing characteristic peaks at 697.3, 776.1, 881.31, and 1070.6 cm−1, which originate from SrCO3; meanwhile, five peaks at 142.7, 200.2, 397.4, 513.3, and 636.7 cm−1 are attributed to TiO2, indicating the existence of Ti and Sr in Ti0.5Sr0.5O3 as shown in Fig. 1c.19 The peaks at 142.7, 200.2, and 636.7 cm−1 correspond to the Raman prominent E1g, E2g, and A3g symmetric stretching modes of titanium oxygen bonds.20 The low-frequency bands at 397.4 and 513.3, attributed to B1g + A1g, correspond to symmetric modes.21 The lateral peak at 636.7 cm−1 shows an atomic configuration that corresponds to the monoclinic C2/m phase, in which the Ti atoms are linked to equatorial oxygen atoms. Raman analyses confirm that the monoclinic enhancement is a consequence of molecular chaotic behaviour caused by the uncertain configuration. In the course of solid-state reactions, changes in thermal effect and weight will occur.22 These modifications will correspond to the formation and composition changes of the nano step-shaped facet that occur during the heating process. The thermal effect and weight changes will occur simultaneously. As a result, TGA and DTG were combined to perform a complete thermal study, as depicted in Fig. 1d. The initial weight loss happened when Ti0.5Sr0.5O3 was heated from 50 to 400 °C due to the loss of hydroxyl molecules.23 This could be attributed to the dehydration of absorbed fluids, as well as the disintegration of unreacted monomers and impurities in the sample.24 Furthermore, the DTG curve revealed that the characteristic weight growth occurred at around 140 °C. The upward-projecting peak in the graph is assumed to represent the growth pattern of the nano step-shaped crystal facet. This is a hypothesis that has been advanced. When N2 is subjected to the whole thermogravimetric test procedure, the weight rise at 160 °C is attributable to the entrance of an element into the lattice during crystal surface recombination. The curve returns to normal after 300 °C, indicating that N2 is released from the lattice. The nanosphere forms during this process. According to the TGA–DTG findings, the temperature at which step-shaped crystal facet formation occurs is between 200 and 400 °C, which is also the temperature at which sphere surface reformation occurs.25
The porosity of Ti0.5Sr0.5O3 has been examined employing the Brunauer–Emmett–Teller (BET) gas adsorption experiment. Fig. S6 reveals Ti0.5Sr0.5O3 has type-IV isotherms with a discrete hysteresis loop. The size distribution curves illustrated mesoporosity, with several small and medium porous structures. The BET surface area of Ti0.5Sr0.5O3 is 181 m2 g−1, with an average pore radius of 17.7 Å. The Ti0.5Sr0.5O3 composite's high surface area and rich mesoporous structure allow for electrolyte access with active spots. The Ti0.5Sr0.5O3 composite has a large surface area, pore volume (0.29 cc g−1), and pore radius, permitting for a rapid electrolyte approach and effortless access to reactants with potential active sites.
As shown in Fig. 2a–d, the Ti0.5Sr0.5O3 particle with a solid sphere structure is seen from the section of particles after calcinating the sample at 400 °C. Fig. S2 shows the resulting EDX profile. Peaks for titanium, strontium, carbon, and oxygen are present.26 The calculated quantities of Ti, Sr, and O are 49.96, 38.87, and 11.7 wt%, based on the EDX profile's peak intensities. The determined number of metals in the sample is nearly identical to the TG analysis results, with only a slight change. Fig. 2i–l shows how elemental mappings supported the EDX study results. The elemental mappings clearly show the existence of all three elements (Ti, Sr, and O) with a uniform distribution, suggesting that the stoichiometry and stability of the bulk material are maintained. Notably, the intensities of Sr and Ti are higher, indicating that the processed sample is largely constituted of Ti0.5Sr0.5O3. Fig. 2e and f demonstrates its high-resolution transmission electron microscopy (HRTEM) illustrations of Ti0.5Sr0.5O3 nanosphere. Fig. 2g shows that the Ti0.5Sr0.5O3 nano spherical sample exhibits two-dimensional lattice fringe patterns, implying that the nanocomposite is crystalline.27 As expected, the estimated interplanar spacing values of about 0.08, 0.8, and 0.20 nm correlate to the (221), (002), and (212) planes of Ti0.5Sr0.5O3, respectively, that is precisely indexed with C/2m symmetry, indicating a spherically [002] Ti0.5Sr0.5O3 phase. The Fast Fourier Transformation (FFT) of the HRTEM brings up the lattice fringe image, predicts the absence of defect and distortion, implying that Ti0.5Sr0.5O3 has a high-quality crystal structure, the existence of all three elements (Ti, Sr, and O) with a uniform distribution, suggesting that the stoichiometry and stability of the bulk material are maintained. These faults were represented in the intensity of the XRD spectra, as well as in the homogeneous atomic distribution. Fig. 2h demonstrates the nanosized spherical Ti0.5Sr0.5O3 nanoparticles through the SAED pattern. It displayed diffraction corresponding to (113), (221), (202), (002), and (213) planes of the Ti0.5Sr0.5O3. Whereas the Ti0.5Sr0.5O3 material has been ground into powder for this efficient evaluation, the image indicates an extensive number of spherical particles, thus being consistent with the SEM conclusions. The depicted pattern is distinguished by well-defined dots, which comprise clearly defined points and spirals, which validates the nanocomposites.28 Additionally, the low defect concentration plays a significant role in frequent electron transport and also in titanium and strontium-ion insertion/extraction within the material.
The XPS spectra of TiSrO3 in Fig. 3 show the predicted elemental states of the crystalline oxide. From Fig. 3b, the Ti 2p spectra demonstrated Ti4+ peaks at ∼458 eV (Ti 2p3/2) and ∼463 eV (Ti 2p1/2), revealing a spherical Ti–O lattice. A slight peak with lower binding energy indicates the presence of relatively small Ti3+ species, apparently due to oxygen vacancies. From Fig. 3c, the Sr 3d spectra exhibit doublet peaks at ∼132.0 eV (Sr 3d5/2) and ∼135 eV (Sr 3d3/2), showing lattice Sr2+. A slightly higher binding energy contribution is attributed to surface hydroxylation or carbonate production. From Fig. 3d, the oxygen 1s spectrum can be separated into lattice oxygen (∼529 eV) and surface hydroxyl groups (∼531 eV), with a minor contribution from carbonate molecules (∼532.5 eV).
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| Fig. 3 XPS spectra; (a) XPS full survey spectra of Ti0.5Sr0.5O3, (b) Ti 2p, (c) Sr 3d, (d) O 1s, and (e) C 1s. | ||
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| Fig. 4 (a) LSV curves; (b) comparison of the overpotential; (c) Tafel plots; (d) stability analysis; (e) Nyquist plot of Ti0.5Sr0.5O3/NF. | ||
| OH− + * → OH* + e− |
Step II: formation of O*:
| OH* + OH− → O* + H2O + e− |
Step III: *OOH formation (rate-determining step):
| O* + OH− → OOH* + e− |
Step IV: oxygen release:
| OOH* → O2 + * + H+ + e− |
The synergistic interaction of Ti0.5Sr0.5O3/NF surface, electrostatic, and structural properties resulted in its enhanced catalytic effectiveness in the hydrogen and oxygen evolution reaction. The electronic structure of the Ti sites, which are the principal active centers for hydrogen adsorption, is impacted by the surrounding oxygen framework and oxygen vacant spaces, which introduce Ti3+ states and raise the electron density at the active sites. Although they are not actively involved in hydrogen binding, the Sr atoms assist with stabilizing the lattice, modulating the covalency of the Ti–O bond, and influencing the perovskite's ultimate electronic conductivity, which promotes charge transfer throughout the reaction. In addition, hydroxyl groups and surface oxygen vacancies enhance water adsorption and dissociation, especially within alkaline conditions, minimizing the Volmer step's activation energy. These elements work together to generate near-optimal hydrogen adsorption free energies, lower reaction barriers, and improved electron mobility, all of which expedite the evolution of hydrogen. In contrast to stoicism of or vacancy-deficient surfaces alone, TiSrO3 exhibits better electrocatalytic activity due to the synergy of structural stability, electronic variability, and surface reactivity.
To accomplish 10 mA cm−2, Ti0.5Sr0.5O3/NF required a minimum overpotential of 299 mV, in contrast with 525 mV for RuO2 and 545 mV for pristine NF, as shown in Fig. 4b, which emphasizes the beneficial effect of thermal treatment on the performance of the catalyst.32 Tafel slope computations in Fig. 4c proved a substantial reduction in slope for Ti0.5Sr0.5O3 as 152.5 mV dec−1, in contradiction to RuO2 as 246.1 mV dec−1 and NF as 288.6 mV dec−1. It therefore implies that Ti0.5Sr0.5O3/NF demonstrates greater effectiveness of charge transfer and increased oxygen evolution kinetics, perhaps due to the resulting synergistic electronic interactions involving the Ti and Sr instances acquired during calcination over time. Due to the high conductivity of the electrolyte, the ohmic drop (iR) was negligible, and therefore compensation was not applied. The stability was tested after an initial 20-minute activation at 200 mA cm−2. Chronoamperometry was employed to determine the longevity of the Ti0.5Sr0.5O3/NF catalyst over 40 hours at a current density of 200 mA cm−2, as illustrated in Fig. 4d. To further explore the diffusion of ion kinetics, electrochemical impedance spectroscopy (EIS) was employed. The precise longitudinal intercept in the region of high frequencies retrieves an indication of series resistance (Rs), which is the combined value of the resistance of the electrolyte, the inherent resistance of electrode material, and the resistance encountered during contact at the active material interface.33 The Nyquist curve, as shown in Fig. 4e, demonstrates charge transfer resistance (Rct), and the straight line depicts quasi-diffusion. Ti0.5Sr0.5O3/NF, which exhibits lower charge transfer resistance (Rct) and greater permeability at the electrode–electrolyte contact. Furthermore, the ECSA, as measured by double-layer capacitance (Cdl) about 2.05 mF cm−2 as shown in Fig. S3c, using CV profile in Fig. S3a, indicates a greater exploitable surface area and increased activity sites for the OER process. High-temperature annealing yields porous nanomaterials, and the improved roughness of the surface has been responsible for this enhancement.
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| Fig. 5 (a) LSV curves; (b) Tafel plots; (c) Nyquist plot; (d) stability analysis of Ti0.5Sr0.5O3/NF. | ||
| Ti site + H2O + e− → Ti–H* + OH− |
Step 2: hydrogen evolution:
Heyrovsky pathway:
| Ti–H* + H2O + e− → H2 + OH− + Ti |
The Nyquist plots in Fig. 5c demonstrate that Ti0.5Sr0.5O3 has the lowest charge transfer resistance of Ti0.5Sr0.5O3/NF, which corresponds to its higher electrical conductivity and surface interaction dynamics. The electrochemical double-layer capacitance (Cdl) was measured using cyclic voltammetry (CV) in the non-faradaic potential range for determining the catalysts' electrochemical surface area (ECSA). CVs were computed at scan rates of 40, 80, 120, 120, 140, 160, 180, and 200 mV s−1. The capacitive current density (Δj = janodic − jcathodic at the middle of the non-faradaic window) was plotted versus scan rate, with the slope of the linear fit corresponding to Cdl. Furthermore, Ti0.5Sr0.5O3/NF has the highest electrochemically active surface area of about 2.83 mF cm−2, as evidenced by Cdl values as shown in Fig. S3c and obtained from CV curves as shown in Fig. S3b, indicating a greater number of exploitable sites that are active for HER.35 The Ti0.5Sr0.5O3/NF catalyst's long-term endurance was tested utilizing the chronoamperometry method at a constant voltage for 40 hours at a current density of 200 mA cm−2, as shown in Fig. 5d.
Moreover, from Fig. S4b, the XRD diffraction pattern after stability testing shows that the characteristic reflections of Ti0.5Sr0.5O3 are largely retained, indicating preservation of the bulk spherical structure. From Fig. S4a, the SEM images show that morphology remains generally intact, although slight surface roughening is observed. From Fig. S5a–e, XPS results show surface analysis reveals partial surface hydroxylation and a slight change in Ti oxidation state, suggesting surface reconstruction under water electrocatalytic conditions. These results indicate that while the bulk structure of Ti0.5Sr0.5O3 remains stable, a thin amorphous (oxy)hydroxide layer likely forms at the surface during operation. This behavior is consistent with reported reconstruction phenomena in metal oxide OER catalysts and suggests that Ti0.5Sr0.5O3 acts as a stable pre-catalyst under high current density.
Supplementary information (SI) is available. See DOI: https://doi.org/10.1039/d6ra00224b.
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