Characterization of MFMH and [Cu(MFMH)2Cl2]
The infrared (IR) spectra of MFMH and Cu(MFMH)2Cl2 are depicted in Figure S2. In the case of MFMH, distinct peaks are observed. Notably, the peak at 3404 cm− 1 is attributed to the stretching vibrations of the N–H bond from the amide group [31–33]. The stretching vibration of C = O appears at 1664 cm− 1 for MFMH and at 1660− 1 for the Cu(MFMH)2Cl2, respectively. Additionally, the stretching vibration of N-N is noted at 935 cm− 1 for MFMH and at 948 cm− 1 for Cu(MFMH)2Cl2, respectively. Furthermore, the stretching vibration of copper-chloride bond (ν(Cu-Cl)) appears at 750 cm− 1.
The analysis of the electronic spectra of NFMH and Cu(MFMH)2Cl2 shown in Figure S3 reveals valuable information about the structural and electronic characteristics of the molecules under study. In the case of the MFMH, we observe the presence of a band with an absorption maximum at 358 nm, which can be attributed to the n-π* transition of the C = O bond. This transition is an indication of the presence of the imide group functionality in the molecule, providing information about its chemical structure.
On the other hand, when analyzing the electronic spectrum of the Cu(MFMH)2Cl2 complex, we notice the presence of two distinct bands with maxima at 385 nm and 401 nm. These bands can be attributed to the n-π* and π→π* transitions of the imine group, respectively. These transitions indicate the presence of the imine group in the complex and suggest a change in the electronic structure of the bonds within the molecule compared to free MFMH.
This information is crucial for understanding the molecular interactions and structural changes that occur when forming the copper complex. Furthermore, these electronic transitions can play an important role in the catalytic properties of the complex, making this data essential for the study of its electrocatalytic activity in ethanol oxidation.
From the theoretical calculations, we observe that octahedral metallic center oriented the acylhydrazone ligands at equatorial position, meanwhile the chloride anions are displaced at longitudinal axes, keeping the compound symmetry at C2 point group, as shown at Fig. 1.
The TDDFT calculations showed the states associated with the absorption bands, considering the Cu(MFMH)2Cl2 at alcoholic milieu. At Fig. 2a is possible to see a little band at the near infrared region which are associated at ß HOMO-1 (π orbitals from ligands) → ß LUMO (σ* orbital at metallic center).
From Fig. 2b is possible to see that mainly three states are associated with bands 3at visible spectrum. The very frst state (420 nm) is associated at electronic transition occurred from π→ π* at ligands. Our data suggest that transition depicted at Fig. 3 is twice representative than the transition showed at Fig. 4. This last transition, also have a small metal-to-MFMH σ* character.
Our calculations demonstrated that 477 nm band is ruled by metal-ligand bond situation. At Fig. 5, is depicted the σ* orbital (between metallic center and its ligands) where electron departures to π de-localized orbitals at MFMH ligands. This transition is also responsible (in part) for 514 nm band.
There is also a π back-donation (Fig. 6) that comes from both, molecular phenyl portions and localized Lewis pairs of chloride ligands, arriving at internuclear regions (σ*) between copper center and all ligands.
As mentioned before, the 514 nm band is composed majoritarily by the transition depicted at Fig. 5, and minoritarily by the the transition depicted at Fig. 7, which have some π → π * characteristic.
Considering the MFDF ligand, our calculations showed that the main light absorption occurred at 355 nm, 385 nm, and 642 nm Figure S5. These excitations are due HOMO → LUMO + 1 transition (Figure S6), HOMO-1 → LUMO transition (Figure S7), and HOMO → LUMO transition (Figure S8).
The thermal stability of MFMH, Cu(MFMH)2Cl2, and CPE-30% was characterized by the thermogravimetric analysis (TGA). The data from Thermal Gravimetric Analysis are shown in Figure S9.
MFMH exhibited two decomposition stages, with the first attributed to a 5% mass loss of the solvent and the second corresponding to 93.87% of the molecule's mass. The complex displayed a two-stage decomposition pattern only. The first stage is attributed to the elimination of water or solvent, and the second stage to the loss of one ligand molecule. It is worth noting that within the experiment's temperature range (30°C to 600°C), approximately 52% of residual mass remained. There was no weight loss indicating the presence of coordinated water molecules in the complex.
For CPE 30%, the decomposition pattern showed two stages, with the first related to solvent and/or nujol loss, which was used in the carbon paste preparation, and the second, more pronounced, linked to ligand loss. In terms of thermal stability, we observed that among the three compounds, the carbon paste was the most stable, followed by the complex, and lastly, the MFMH ligand. It is highly likely that the inclusion of graphite increases stability, resulting in a higher residual mass.
The cyclic voltammogram of MFMH displays an irreversible oxidation process at 1.29 V and a reduction process at -0.74 V, corresponding to electrochemical processes characteristic of the molecule itself. The oxidative process remains unchanged after complexation with the Cu(II) metal ion. However, at a scan rate of 10 mV/s, in the cathodic region, two processes are observed at -0.86 V and − 1.05 V, attributed to the ligand and the reduction of Cu(II) to Cu(I), as shown in Figure S4.
Electrochemical analysis
Eletrocatalytic experiments on ethanol oxidation.
Figure 8: Cyclic voltammogram in acidic medium (0.5 mol L-1 H2SO4) in the presence of ethanol (1.0 mol L-1) for Cu-CPE 30% and Cu(MFMH)2Cl2 (insert) both at a scan rate of 10 mV s-1 and 25°C.
As differences observed in the cyclic voltammograms between Cu(MFMH)2Cl2 in solution and Cu-CPE 30% in the presence of ethanol in an acidic medium are significant and indicate crucial differences in the electrochemical behavior of these materials.
In the cyclic voltammogram of Cu(MFMH)2Cl2 in solution, it can be observed that the current remains close to zero around the potential of 0.4V in the presence of ethanol. This indicates that, at this specific potential, there is no significant ethanol oxidation occurring. This response is typical of a material that does not act as an efficient catalyst for ethanol oxidation. On the other hand, in the cyclic voltammogram of Cu-CPE 30%, under the same acidic pH conditions and in the presence of ethanol, a clear ethanol oxidation is observed around the potential of 0.4V, as evidenced by the substantial increase in current in this region. This suggests that Cu-CPE 30% is an effective catalyst for ethanol oxidation, allowing this reaction to occur at a lower potential.
pH variation
We investigated the behavior of the Cu-CPE 30% catalyst in an acidic environment at pH values of 1.16, 1.44, 1.93, 2.81, and 5.44 in relation to the electrocatalytic oxidation of ethanol, as shown in Fig. 9.
The voltammograms of ethanol electrocatalytic oxidation at different pH values reveal a correlation between pH and catalytic performance. The analysis of the catalytic system at various pH levels indicates that maximum efficiency is achieved at pH 1.16, decreasing as pH increases and reaching a minimum at pH 5.0. This suggests that the increased concentration of H + ions facilitated the electrocatalytic oxidation by removing adsorbed intermediates. This result was confirmed through chronoamperometry at different concentrations. However, there is a limit, as no current was obtained when cyclic voltammetry was conducted at pH 0.9, indicating that the paste is not stable under these conditions.
Variation in ethanol concentration
We investigated the electrocatalytic oxidation of ethanol catalyzed by Cu-CPE 30% through cyclic voltammetry and chronoamperometry at different ethanol concentrations (0.1; 0.2; 0.4; 0.6; 0.8; and 1.0 mol L− 1), as illustrated in Figs. 10a-b.
The results were obtained in an environment with a pH of 1.16 and ethanol, applying an anodic potential of 0.6 V versus the Ag/AgCl reference electrode. These experiments allowed us to determine catalytic activity at a constant potential over a specific time period, thus eliminating transient phenomena associated with variations in the electric field of the electrodes. In other words, we measured only the average rate of alcohol electro-oxidation under investigation.
When analyzing the chronoamperometry results, we observed a clear trend where the current density decreases as the ethanol concentration is reduced. This direct decrease in current density can be attributed to the adsorption of the adsorbate on the surface of the electrocatalyst.
As the ethanol concentration decreases, there are fewer ethanol molecules available at the electrode-solution interface. This results in a lower rate of adsorption of these molecules on the surface of the electrocatalyst. The adsorption of ethanol is a crucial step in the electrocatalytic oxidation reaction of this compound, and the reduction in the availability of ethanol on the catalyst's surface can negatively impact the reaction rate.
Therefore, the decrease in current density observed with decreasing ethanol concentration suggests that the adsorption of the adsorbate on the electrocatalyst's surface plays a crucial role in the kinetics of the ethanol oxidation reaction. This highlights the importance of understanding the interaction between the reacting species and the catalyst's surface when designing electrocatalytic systems for ethanol oxidation at different concentrations.
Temperature variation
To investigate the performance of the Cu-CPE 30% catalyst at different temperatures, we conducted cyclic voltammetry in an ethanol medium (1.0 mol L− 1) at a pH of 1.16. The evaluated temperatures were 24.5°C, 30°C, 40°C, 50°C, and 60°C, as shown in Fig. 9b.
We observed that the peak current for ethanol oxidation exhibited a gradual and direct increase with the rise in the system's temperature within the range of 24.5°C to 50°C. This behavior aligns with theory, as elevated temperatures typically promote faster and more efficient chemical reactions, including electrochemical processes.
However, when the system temperature reached 60°C, we noticed a significant decrease in the peak current for ethanol oxidation. This decline can be attributed to various factors, such as electrode stability and potential alterations in the adsorption of reactant species on the electrode's surface, as well as changes in reaction kinetics. Additionally, higher temperatures can lead to increased volatility of ethanol, which might affect its availability at the electrode-solution interface.
In summary, our findings suggest that the performance of the Cu-CPE catalyst in ethanol oxidation is directly linked to the system's temperature. Nevertheless, there appears to be a threshold beyond which excessively high temperatures can adversely impact the efficiency of the electrochemical reaction.
Considering that long-term structural stability is equally critical for electrocatalysts [13, 15], we assessed this property for the Cu-CPE catalyst. This was done through continuous cyclic voltammetry, ranging from 0.05 V to 1.1 V, in a pH 1.16 environment, using a 1.0 mol L-1 ethanol solution, all at room temperature (Fig. 13).
When analyzing the cyclic voltammetry data obtained with Cu-CPE 30%, we observed an intriguing phenomenon related to the peak current for ethanol oxidation. As we increased the number of cycles, a significant increase in current density was noticeable after 20 cycles compared to the first cycle.
This rise in current density strongly implies that the modified electrode maintained its electrochemical catalytic activity throughout these repeated cycles. In other words, the electrode exhibited stability under test conditions, a crucial characteristic for its application as an effective electrocatalyst.
The fact that the current density increased approximately tenfold after 20 cycles in the ethanol oxidation region (0.25 V) indicates that the modified electrode did not undergo significant degradation during the test, which is a positive indicator of its durability and ability to maintain consistent performance over time.
These findings hold promise for the practical application of the modified electrode in ethanol oxidation systems, as they suggest that it can deliver stable and reliable performance under continuous usage conditions.