Saad G.
Mohamed
*ab,
Jixu
Wan
c and
Xuejin
Li
*c
aMining and Metallurgy Engineering Department, Tabbin Institute for Metallurgical Studies (TIMS), Tabbin, Helwan 109, Cairo 11421, Egypt. E-mail: saadmohamed@tims.gov.eg
bAcademy of Scientific Research & Technology (ASRT), 101 Kasr Al-Ainy St., Cairo, Egypt
cSchool of Materials Science and Engineering, State Key Laboratory of Heavy Oil Processing, China University of Petroleum (East China), Qingdao, 266580, P. R. China. E-mail: lxjupc@gmail.com
First published on 7th November 2024
The quest for sustainable energy storage has spotlighted zinc-ion batteries (ZIBs) for their safety, cost-effectiveness, and eco-friendliness. Manganese oxides, particularly Mn3O4, stand out as promising cathode materials due to their electrochemical virtues and affordability. However, traditional synthesis methods like solid-state reactions, hydrothermal processes, and sol–gel techniques often entail complex procedures, high temperatures, and environmentally harmful chemicals, which impede their practical applications. This study introduces a novel, eco-friendly synthesis route for Mn3O4 nanoparticles via the room-temperature reaction of morpholine with manganese nitrate for 24 h, reducing both the environmental impact and the complexity of production. This method yields Mn3O4 nanoparticles with enhanced crystallinity and surface area, which is crucial for improved electrochemical performance in ZIBs by offering increased active sites for zinc intercalation. The resultant high-performance Mn3O4 nanoparticles align with sustainable practices and hold the potential for advancing next-generation energy storage technologies. The detailed structure and electrochemical performance were investigated in detail in this study. The produced Zn//Mn3O4 nanoparticles cell exhibited a remarkable electrochemical performance, which displayed a high reversible capacity of 209.7 mAh g−1 after 300 cycles at 0.6 A g−1.
Manganese oxides, particularly Mn3O4, have been extensively studied as cathode materials for energy storage applications due to their abundance, low cost, and favorable electrochemical properties.6–8 Mn3O4 has emerged as a promising candidate for use in aqueous ZIBs owing to its ability to provide a balance between both considerable capacity and high voltage.9,10 However, like other manganese-based oxides, Mn3O4 suffers from capacity degradation and suboptimal rate performance, primarily attributed to its inherent poor conductivity and the dissolution of Mn2+ ions.11 Traditionally, Mn3O4 has been synthesized through various techniques such as solid-state reactions,12 hydrothermal processes,13 and sol–gel methods,14 each requiring multiple steps, high temperatures, or the use of hazardous chemicals.
The solid-state reaction method, while effective in producing Mn3O4, often involves prolonged heating at high temperatures, leading to large particle sizes and reduced surface area, which can negatively impact the material's electrochemical performance. Hydrothermal and sol–gel methods, on the other hand, typically require the use of surfactants or organic solvents to control the morphology and particle size of Mn3O4, introducing additional steps and potential environmental concerns. Although successful in producing Mn3O4, these conventional methods often involve complex synthesis procedures and non-eco-friendly reagents, which can limit their scalability and sustainability.
In this study, we explore a novel and green synthesis route for Mn3O4 using the reaction of morpholine with manganese nitrate at room temperature. This method significantly reduces the number of synthesis steps and avoids the use of high temperatures or hazardous chemicals, making it an environmentally friendly alternative to conventional techniques. Morpholine, acting as both a complexing agent and a base, facilitates the controlled precipitation of manganese hydroxide, which is then oxidized to Mn3O4 in a single step under mild conditions. This synthesis approach not only simplifies the production process but also yields Mn3O4 with a high crystallinity and surface area, which is critical for enhancing the electrochemical performance of ZIBs by providing more active sites for Zn2+ intercalation. Moreover, using this green synthesis method aligns with sustainable chemistry principles, offering a more straightforward and eco-friendly approach to producing high-performance Mn3O4. The resultant Mn3O4 exhibits high performance in ZIBs, making it an attractive material for next-generation energy storage devices. By reducing the complexity and environmental impact of the synthesis process, this study contributes to the advancement of sustainable materials for energy applications.
Fig. 1 (a) XRD pattern, (b) Raman spectrum, (c) Mn 2p XPS high-resolution spectrum, and (d) O 1s XPS high-resolution spectrum of the produced Mn3O4 nanoparticles. |
The as-prepared Mn3O4 nanoparticles exhibit strong diffraction peaks at 2θ degrees (with the corresponding lattice planes) of 17.99 (101), 28.96 (112), 31.00 (200), 32.32 (103), 36.04 (211), 38.08 (004), 44.53 (220), 49.91 (204), 50.76 (105), 53.96 (312), 56.12 (303), 58.62 (321), 59.86 (224), 63.17 (116), 64.62 (400), 67.64 (411), 69.71 (305), 74.21 (413), 76.73 (422), and 77.64 (422). No further crystalline phases were found, and the significant diffraction peaks in patterns detected by XRD show that the resultant product is highly crystallized.
Furthermore, the Raman spectrum distinctly exhibits the characteristic signatures of crystalline Mn3O4. Notably, three pronounced vibrational peaks are observed (Fig. 1c) at 316, 370, and 663 cm−1, corresponding to the Eg, T2g, and A1g active modes of Mn3O4, respectively. The most intense peak is attributed to the Mn–O stretching vibration of tetrahedral Mn2+ within the spinel Mn3O4 structure. The two less intense peaks are associated with the combined vibrational modes of oxygen atoms in both tetrahedral and octahedral sites.15–17 The X-ray photoelectron spectroscopy (XPS) analysis of the Mn 2p region for Mn3O4 nanoparticles reveals a complex valence (mixed valence) state for manganese, as depicted in Fig. 2c. The binding energy peaks at 642.18 eV and 653.68 eV correspond to Mn 2p3/2 and Mn 2p1/2, respectively. The spectral peaks can be deconvoluted to features at 641.18 eV and 652.9 eV, which are attributable to Mn2+, while those at 642.68 eV and 653.68 eV align with Mn3+, and the peaks at 644.48 eV and 655.28 eV are indicative of Mn4+.18 The occurrence of Mn4+ may also suggest surface oxidation processes, potentially converting Mn2+ to Mn3+ within Mn3O4.18,19Fig. 2d presents the deconvoluted O 1s XPS spectrum for Mn3O4 nanoparticles synthesized via a green method. Three distinct binding energies are identified: 529.9 eV, 531.6 eV, and 532.7 eV. These are respectively attributed to the Mn–O–Mn linkages in the tetravalent oxide, oxygen defects and/or Mn–OH bonds, and H–O–H of adsorbed water molecules.17,19,20
Fig. 2 (a) SEM image, (b) TEM Image, (c) SAED, and (d) Nitrogen adsorption and desorption isotherm (inset shows the pore distribution) of the produced Mn3O4 nanoparticles. |
The MnO3O4 formation mechanism can be described as follows: the reaction of morpholine (O(CH2CH2)2NH) with manganese nitrate (Mn(NO3)2) aqueous solution at room temperature can be stepwise ascribed by the following steps: 1-dissolution of Mn(NO3)2 in water forms Mn2+ and NO3− ions. 2-Morpholine acts as a multifunctional agent, serving as both a complexing agent and a base. 3-Mn(OH)2 and Mn(OH)3 form due to an increase in pH from morpholine, which can further dehydrate and oxidize to form Mn3O4. The following equation describes the possible mechanism of the reaction between manganese nitrate and morpholine in an aqueous solution.
Mn(NO3)2 → Mn2+ + 2NO3− |
Mn2+ + O(CH2CH2)2NH → [Mn(O(CH2CH2)2NH)]2+ |
O(CH2CH2)2NH + H2O → O(CH2CH2)2NH2+ + OH− |
Mn2+ + 2OH− → Mn(OH)2↓ |
Mn2+ + NO3− + H2O → Mn3+ + NO2− + 2OH− |
Mn3+ + 3OH− → Mn(OH)3↓ |
2Mn(OH)3 + Mn(OH)2 + NO3− → Mn3O4 + NO2− + 3H2O + 2OH− |
The following equation can describe the overall reaction;
3Mn(NO3)2 + 4O(CH2CH2)2NH + 2H2O → Mn3O4 + 4O(CH2CH2)2NH2+ + 6NO2− + 4OH−
The morphological characteristics of the synthesized Mn3O4 nanoparticles were thoroughly examined through scanning electron microscopy (SEM). As represented in Fig. 2a, the Mn3O4 nanoparticles are composed of uniformly distributed micron-sized aggregates, with individual particle sizes ranging from approximately 10 to 60 nm with porous features, as illustrated in transmission electron microscope image (TEM), Fig. 2b. The nanoparticles exhibit an irregular morphology, which is indicative of a potentially large specific surface area. This structural feature is anticipated to contribute favorably to their electrochemical performance. The high degree of crystallinity (polycrystalline nature) is clearly evidenced by the well-defined SAED pattern shown in Fig. 2c. The structure is expected to offer an ample contact area for electrolyte permeation while also providing a sufficient number of active sites to facilitate the insertion and extraction of Zn2+ ions. In Fig. 2d, the N2 adsorption/desorption isotherms and the corresponding pore size distributions (shown in the inset) are presented. The isotherms exhibit characteristics typical of type IV, which are commonly associated with the mesoporous nature of Mn3O4 nanoparticles. Notably, the surface area of the Mn3O4 nanoparticles was measured to be 28.8 m2 g−1. The analysis of pore size distributions reveals that a significant portion of the pores in the Mn3O4 nanoparticles fall within the mesoporous range. This finding suggests that the produced Mn3O4 nanoparticles contain a considerable number of pores with diameters consistent with mesoporous structures.
Cyclic voltammetry (CV) and galvanostatic charge–discharge (GCD) tests were performed to evaluate the electrochemical behavior and performance of Mn3O4 nanoparticles. Fig. 3a presents the first six CV curves of Mn3O4 nanoparticles electrode at a scan rate of 0.1 mV s−1, where two distinct pairs of redox peaks are observed at 1.25/1.38 V (cathodic scan) and 1.56/1.60 V (anodic scan). During the discharge process, the reduction peaks at 1.38 V and 1.25 V correspond to the insertion of H+ and Zn2+ ions, respectively, along with the reduction of Mn3+ to Mn2+ and Mn4+ to Mn3+.18,19,21 In the charging process, the oxidation peaks at 1.56 V and 1.60 V are associated with the extraction of Zn2+ and H+ ions,22 accompanied by the oxidation of Mn2+ or Mn3+ to Mn3+ or Mn4+.18,19 The increasing peak current intensity by the cycling could be that during the initial charge process, the Mn3O4 phase transforms into an intermediate Mn5O8 phase. Subsequently, as Mn2+ ions dissolve, the Mn5O8 phase gradually converts into spinel-layered MnO2. Also, as Mn5O8 transitions into MnO2, the intensity of the reduction peaks progressively increases.23
As illustrated in Fig. 3b, during the initial charge–discharge cycles at a current density of 0.2 A g−1, the Mn3O4 nanoparticles electrode demonstrated a progressive increase in capacity. Notably, the charge/discharge capacity started at 94.0/75.7 and reached the high value of 778.7/767.4 mAh g−1 at cycle number 37. This phenomenon can be attributed to the typical activation process observed in manganese-based cathodes when operating in an aqueous electrolyte.22,24 After cycle 40, fluctuations in the capacity trend were observed. The electrode maintained a reversible capacity of 689.3 mAh g−1 by continuous cycling, which can be attained in the 50th cycle. The coulombic efficiency (CE) remained consistently around 99% throughout the multiple cycles.
Fig. 3b′ inset depicts the Mn3O4 nanoparticles cathode charge–discharge profile based on the selected cycles in Fig. 3b. Remarkably, the discharge profile displays two distinct plateaus at 1.25 to 1.3 V and 1.4 to 1.5 V, corresponding to the insertion of H+ and Zn2+ ions into the Mn3O4 matrix. The plateaus observed at approximately 1.55 V and 1.65 V in the charge profiles are associated with extracting H+ and Zn2+ ions from the Mn3O4 hosts. These findings agree with the two pairs of redox peaks observed in the CVs. Similar behavior has been reported in Mn3O4 electrodes as ZIB cathode.25,26
As illustrated in Fig. 3c, the rate-capacity results demonstrate a gradual decline in reversible capacity with increasing current densities. At a current density of 0.6 A g−1, the charge/discharge capacity progressively increases after 15 cycles to 219/217.8 mAh g−1. The Mn3O4 nanoparticles electrode delivered charge/discharge capacities of 186.3/184.3, 146.8/146.2, 79.3/79.1, and 30.9/30.5 mAh g−1 at current densities of 0.8, 1, 2, and 5 A g−1, respectively. However, when the current density is reduced again in the same trend from 5 A g−1 to 0.6 A g−1, the reversible capacity is restored to 74.3/74.5, 147.0/154.0, 187.6/194.6, and 212.7/211.1 mAh g−1, as the current density reversed to 2, 1, 0.8, and 0.6 mA g−1, respectively, exhibiting superior rate performance, which could be ascribed to the large specific surface area and the porous feature of the Mn3O4 which facilitates the efficient insertion and extraction of Zn2+ ions during the discharge–charge processes, further contributing to its improved electrochemical performance.
Moreover, Fig. 3d demonstrates the long-term cycling stability at a current density of 0.6 A g−1. It is observed that the specific capacity gradually increases with the progression of cycling, which is attributable to the material activation. This activation arises primarily from two factors: (1) the infiltration of the electrolyte into the cathode enhances the reversible reactions and minimizes the electrochemical inactivity of the active materials, and (2) the synergistic interaction between Zn2+ and Mn2+, coupled with the redox reaction of Mn2+, necessitates time for diffusion from the electrolyte into the bulk phase of the positive material.18,27 The capacity of the electrode demonstrates a gradual increase throughout the cycling process, culminating in a higher charge/discharge capacity of 209.7/209.1 mAh g−1 after 300 cycles.
To gain a more comprehensive understanding of the dynamic mechanisms involved in Zn//Mn3O4 cell during charge storage, cyclic voltammetry (CV) was conducted at varying scan rates. As observed in Fig. 4a, an increase in scan rate results in a shift of the reduction peaks toward lower potentials and the oxidation peaks toward higher potentials, indicative of enhanced polarization. Additionally, the current intensity of peak 2 and peak 3 becomes significantly more noticeable, which can be attributed to the fact that with increasing current, the reaction process becomes progressively dominated by H+ insertion.19 The relationship between the current (i) and scan rate (v) can be expressed using the equation i = avb, where b values of 0.5 and 1.0 correspond to diffusion-controlled and pseudocapacitance-controlled reactions, respectively.28,29 The calculated b values for peaks 1, 2, and 3 of Zn//Mn3O4-nanoparticles cell, as determined from the correlation between log(i) and log(v) (Fig. 4b), are 0.885, 0.796, and 0.976, respectively. The raised b values observed for the Mn3O4 nanoparticles electrode suggest pronounced pseudocapacitive properties similar to those found in the previous related Mn3O4-base electrodes,18,19 which indicates a substantial rate performance.
Fig. 4 (a) CV curves of Mn3O4 nanoparticles cathode at different scan rates, (b) logi and logv plots resulted from Fig. 4a, (c) the capacitive/diffusion contribution ratios in Mn3O4 nanoparticles cathode electrode, (d) capacitive contribution to the total capacity at a scan rate of 0.1 mV s−1, and (e) cycling performance operated at −10 °C at 0.2 A g−1 and inset is discharge/charge profiles of the cycle number 1500. |
Additionally, the contributions from capacitive and diffusion processes can be differentiated into capacitive-controlled (k1v) and diffusion-controlled (k2v1/2) components, as expressed in the equation: i(V) = k1v + k2v1/2, which can be reformulated as i(V)/v1/2 = k1v1/2 + k2.30 The constants k1 and k2 can be determined by plotting the relationship between i(V)/v1/2 and v1/2, corresponding to the capacitive behavior and diffusion-controlled process.
Fig. 4c illustrates the pseudocapacitance contributions of Zn//Mn3O4-nanoparticles cell with scan rates, recording values of 60.4%, 72.6%, 77.4%, 80.2%, and 82.9% at scan rates of 0.1, 0.3, 0.5, 0.7, and 1 mV s−1, respectively. For instance, the CV profile for the capacitive contribution compared with that of the diffusion-controlled current at 0.1 mV s−1 is around 60.4% capacitive-dominated to 39.6% diffusion-controlled process, as shown in Fig. 4d.
The capacitance characteristics of the electrode exhibit a pronounced increase with rising scan rates, enhancing its capacity to store and release charges at elevated currents. This improvement bestows upon the Zn//Mn3O4-nanoparticles cell superior and preeminent ZIB performance.
Even at a low temperature of −10 °C, the Zn//Mn3O4-nanoparticle cell in a ZnSO4-0.1 M MnSO4-30% 1,2-dimethoxyethane (DME) electrolyte demonstrates a reversible capacity of 50 mAh g−1 with nearly 100% CE after 1500 cycles at a current density of 0.2 A g−1 (Fig. 4d), with charge/discharge profile, shown in Fig. 4d′ inset, is similar to the room temperature profile without DME addition, indicating excellent compatibility at low temperatures. It is noted that the activation process takes longer cycles, which can be attributed to the decrease in the migration rate of ions in the electrolyte, resulting in a substantial reduction in ionic conductivity. This, in turn, directly increases the battery's internal resistance, adversely impacting its charging and discharging performance.31
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ya00539b |
This journal is © The Royal Society of Chemistry 2024 |