3.1 TEM (Transmission Electron Microscopy) Analysis
Figure 1 depicts the results obtained from TEM analysis of Co3O4-AC and Co3O4-SG samples. TEM images (a, d) show the majority of particles exhibiting a spherical morphology, although a few particles appear to have a hexagonal shape. High-resolution TEM images (b, e) provide detailed views of the crystal planes that are exposed. Particle size analysis was performed using Gatan digital micrograph software, and the obtained data was used to generate particle size distribution histograms (Fig. 1(c, f)). The histograms reveal the distribution of particle sizes within each sample. The average particle size was found to be 28 nm for Co3O4-AC and 23 nm for Co3O4-SG. Furthermore, the interplanar distance (d) between crystal planes was measured and found to be 0.243 nm for Co3O4-AC and 0.269 nm for Co3O4-SG, specifically corresponding to the (311) crystal planes.
3.2 XRD (X-Ray Diffraction) Analysis
Figure 2 presents powder XRD patterns obtained for the nanomaterials (NM) prepared by Autocombustion (AC) and Sol-gel (SG) methods. In Fig. 2a, the XRD patterns for Co3O4-AC and Co3O4-SG are displayed, while Fig. 2b shows an enlarged view of the maximum intense peak (311). The XRD patterns of Co3O4-AC and Co3O4-SG samples closely match the simulated pattern of Co3O4 generated from PCW software. This agreement confirms the phase purity of the prepared nanomaterials, as no impurity peaks are observed. Furthermore, the broad peaks observed in the experimental patterns indicate that the crystallites are nano-sized. The crystallite size was calculated using the Debye-Scherrer formula and found to be 44 nm for Co3O4-AC and 36 nm for Co3O4-SG. The interplanar distance (d) for (311) plane was calculated using Bragg's law (nλ = 2dsinθ) and determined to be 0.2433 nm for Co3O4-AC and 0.2432 nm for Co3O4-SG. These values are comparable with the interplanar distances observed in the TEM analysis. The lattice parameter (a) was calculated by relating the (hkl) plane to the interplanar distance (d) and found to be 0.8066 nm for both nanomaterials (Chen et al., 2017; Rani et al., 2017).
3.3 BET (Brunauer–Emmett–Teller)) Analysis
Figure 3 presents the N2 adsorption-desorption isotherms for Co3O4-AC (Fig. 3a) and Co3O4-SG (Fig. 3b). Prior to the analysis, the samples were subjected to a heating process at 120°C for 3 hours to eliminate any moisture or adsorbed gases. The presence of hysteresis loops in the adsorption-desorption isotherms indicates that the prepared samples possess a mesoporous structure. These samples follow a type-IV adsorption/desorption isotherm pattern. The surface area, pore volume, and pore diameter of Co3O4-AC were determined to be 15 m2/g, 0.083 cm3/g, and 22 nm, respectively. In comparison, Co3O4-SG exhibited higher values for surface area, pore volume, and pore diameter, measuring 11 m2/g, 0.20 cm3/g, and 73 nm, respectively. This indicates that Co3O4-AC has a greater surface area and larger pores compared to Co3O4-SG It is important to note that different synthesis methods can lead to variations in surface morphology, thereby affecting the surface area and pore characteristics of the samples.
3.4 X-ray Photoelectron Spectroscopy (XPS) analysis
Figure 4 displays survey spectra of XPS for two nanomaterials, Co3O4-AC and Co3O4-SG, confirming the presence of peaks corresponding to Cobalt (Co) and oxygen (O). The binding energies of high-resolution XPS spectra of Co2p and O1s were corrected using a reference carbon binding energy of 284.6 eV and then deconvoluted. The deconvoluted outcomes are presented in Fig. 5. The emission spectra of Co2p exhibit two-orbit doublets observed at approximately 779.73 eV and 794.68 eV for both samples, representing 2p3/2 and 2p1/2, respectively (Fig. 5a). These values indicate the presence of Co3+ at octahedral and Co2+ at tetrahedral sites within the samples' sublattice. The binding energies (B.E) of both samples, found after deconvolution, are displayed in Table 1, agree well with previous studies (Jang et al., 2017; Zhang et al., 2021). Figure 5b illustrates the deconvoluted high-resolution O1s spectra for both samples, revealing three components: lattice oxygen (OL), oxygen vacancies (OV), and chemically adsorbed oxygen (OC). The primary peak is situated around 529.61 eV and it is accompanied by broadened shoulders at higher B.E. The binding energies of OL, OV, and OC are approximately 529.6, 531.1, and 532.5 eV, respectively. The O1s B.E values for both samples, as shown in Table 2, align well with existing literature (Eismont et al., 2023; Saddeler et al., 2020). This analysis confirms the presence of metal-oxygen (M-O) bonds, specifically Co-O bonding, in both samples.
Table 1
List of Co2p binding energies of the samples.
Sample | 2p3/2 | 2p1/2 |
Co3+ (eV) | Co2+ (eV) | Co3+ (eV) | Co2+ (eV) |
Co3O4-AC | 779.73 | 781.52 | 794.68 | 796.52 |
Co3O4-SG | 779.67 | 781.57 | 794.64 | 796.44 |
Table 2
List of O1s binding energies of samples.
Sample | OL (eV) | OD (eV) | OC (eV) |
Co3O4-AC | 529.61 | 531.16 | 532.56 |
Co3O4-SG | 529.55 | 530.89 | 532.20 |
3.5 Cyclic Voltammetry (CV)
The CV experiments conducted for Co3O4-AC and Co3O4-SG nanomaterials involved varying scan rates such as 5, 10, 25, 50, 75 and 100 mV/s in a three-electrode system using a 1 M KOH electrolyte solution. The obtained CV graphs, shown in Fig. 6, covered a potential window of 0-0.6 V. Both nanomaterials exhibited redox behavior characterized by the presence of anodic and cathodic peaks, indicating their pseudo-capacitive nature. The first pair of redox peaks (A1/C1) can be attributed to the faradaic conversion from Co2+ in Co3O4 to Co3+ (CoOOH), as represented by the equation mentioned previously (Pal et al., 2018; Fan et al., 2019).:
Co3O4 + OH− + H2O ↔ 3CoOOH + e- ………. (1)
The second pair of redox peaks (A2/C2) observed in the CV curves corresponds to the Faradaic conversion between Co3+ (CoOOH) and Co4+ (CoO2), as described by the following equation (Liu et al., 2017):
CoOOH + OH− ↔ CoO2 + H2O + e- ……. (2)
In the case of the Co3O4-AC sample, the migration of peaks observed at higher scan rates can be attributed to the influence of polarization effects and the corresponding increase in internal resistance. These factors contribute to the shifting of the peaks within the cyclic voltammogram. In contrast, the Co3O4-SG sample shows the presence of both redox peaks, and the resulting cyclic voltammograms display a nearly rectangular shape, indicating different electrochemical behavior compared to Co3O4-AC (Li et al., 2020).
3.6 Galvanostatic charge-discharge (GCD)
The GCD curves obtained at various current densities such as 0.25, 0.5, 0.75, 1.0, 2.5 and 5.0 A/g for Co3O4-AC and Co3O4-SG are depicted in Figs. 7a and 7b, respectively. Both samples exhibit two distinct plateaus on the discharging curves, indicating the involvement of redox coupling reactions that were observed in the CV analysis. This behaviour signifies the pseudo-capacitive nature of the materials. Comparing the GCD curves at Im of 0.5 A/g (Fig. 7c), it is evident that the Co3O4-AC sample displays broader GCD curves compared to the Co3O4-SG sample, indicating more charge storage capabilities. This observation is notable considering that Co3O4-AC has higher surface area, pore volume, and pore diameter, as determined in the BET analysis. At a lower Im of 0.25 A/g, the specific capacitance (Cs) values for Co3O4-AC and Co3O4-SG are measured to be 162 F/g and 98 F/g, respectively. However, as the current density increases, the specific capacitance for both materials decreases, as illustrated in Fig. 7d. At all Im, the Cs of Co3O4-AC is considerably higher than that of the Co3O4-SG. This decrease can primarily be attributed to the limited interaction between the electrolyte and the active material present on the electrode surface.
E.D. and P.D. of Co3O4-AC and Co3O4-SG nanomaterials was calculated and results obtained were tabulated seen in Table 3 at different current density. The E.D. decreases and the P.D. increases with the increase in current density from 0.25 A/g to 5.0 A/g. Comparatively, Co3O4-AC shows relatively higher E.D. than the Co3O4-SG nanomaterial.
Table 3
Energy density (E.D) and power density (P.D) values of Co3O4- AC and Co3O4-SG samples, obtained at different current densities.
Current density Im (A/g) | Co3O4 - AC | Co3O4-SG |
E.D (Wh/kg) | P.D (kW/kg) | E.D (Wh/kg) | P.D (kW/kg) |
0.25 | 14.29 | 0.05 | 9.92 | 0.06 |
0.5 | 11.91 | 0.11 | 8.71 | 0.11 |
0.75 | 11.03 | 0.16 | 8.30 | 0.17 |
1.0 | 10.58 | 0.20 | 7.39 | 0.22 |
2.5 | 7.03 | 0.54 | 5.71 | 0.57 |
5.0 | 6.47 | 1.08 | 5.71 | 1.14 |
3.7 Electrochemical Impedance Spectra (EIS)
Figure 8 illustrates the EIS spectra or Nyquist plots obtained for the fabricated Co3O4-AC and Co3O4-SG nanomaterial electrodes. The EIS spectra exhibit distinct characteristics for both electrode materials. In the higher frequency region, a smaller semicircle is observed for the Co3O4-AC sample, while a larger semicircle is observed for the Co3O4-SG sample. This difference in semicircle size suggests that the Co3O4-AC electrode has better charge transport properties at the electrode-electrolyte interface compared to the Co3O4-SG electrode. The point of intersection at the x-axis at the highest applied frequency corresponds to the RS (Ω) or equivalent series resistance (ESR), which represents the total internal resistance of the cell. The RS values were found to be 1.42 Ω and 1.16 Ω for the Co3O4-AC and Co3O4-SG electrodes, respectively. The charge transport resistance (Rct) of the electrode materials can be estimated from the radius of the semicircle, which was determined to be 0.92 Ω for Co3O4-AC and 2.06 Ω for Co3O4-SG. The presence of a vertical line in the low frequency regions indicates the occurrence of ionic diffusion from the bulk of the solution towards the electrode surface. A more vertical straight line suggests lower diffusive resistance of OH− ions. The Co3O4-AC electrode exhibits a more vertical line in the inset of Fig. 8, indicating lower diffusive resistance of OH− ions from the solution towards the electrode surface. This behavior is consistent with studies conducted by Gaire et al. (2020), Ndambakuwa et al. (2021), Hong et al. (2019), Nieto et al. (2021), Ye et al. (2021), and Kharade et al. (2018).
3.8 Stability cycles
The cycle stability of the electrode materials were probed from the charge-dischargecurves recorded up to 1000 cycles under a current density of 5 A/g, and the results are shown in Fig. 9. Both electrode show almost same capacitance retention up to 1000 cycles of experiments. A similar feature of high degree of capacitance retention has been reported for various spinel-structure cobalt oxide systsems (Sharma et al. 2020; Ghosh et al. 2016; Thorat et al. 2017).