Pin-Yi
Zhao
*abc,
Kwang-Leong
Choy
*bc,
Yongyi
Song
a,
Shudong
Zhang
a and
Rui
Ma
a
aSINOPEC (Dalian) Research Institute of Petroleum and Petrochemicals Co., Ltd., 116045, China
bInstitute for Materials Discovery, University College London, WC1E 7JE, UK. E-mail: pinyi.zhao.18@ucl.ac.uk; k.choy@ucl.ac.uk
cDepartment of Chemistry, University College London, WC1H 0AJ, UK
First published on 23rd December 2024
Lithium-ion batteries (LIBs) are essential for energising portable devices, electric cars, and energy storage systems. Graphite is a frequently utilised anode material; nonetheless, the continual formation of a solid electrolyte interface (SEI) during cycling results in capacity degradation owing to electrolyte depletion. This study tackles this issue by employing alumina coatings on graphite electrodes via the spray coating technique, which is cost-effective and scalable. Electrodes with different alumina concentrations (1 wt%, 4 wt%, and 7 wt%) were assessed for electrochemical performance. The 1 wt% alumina-coated electrode demonstrated enhanced cycling stability, with 94.97% capacity retention after 100 cycles, in contrast to 91.74% for the uncoated graphite. The Al2O3 coating functions as a preformed SEI, diminishing electrolyte decomposition and improving the cycling performance and rate capability of electrodes, particularly at elevated C-rates. This research illustrates that using spray-coated alumina is an effective technique for enhancing the durability and performance of graphite anodes in lithium-ion batteries, with the potential for extensive applications in energy storage systems.
Concerted efforts have been undertaken to address this issue. One option involves altering the surface. The coating of Al2O3 operates through the mechanism of the “protection effect”8,9 in which the Al2O3 coatings on graphite have been documented to enhance the safety, cycling, and rate performance of cells.10,11 Al2O3 coatings also serve to safeguard the positive electrode and diminish surface/electrolyte interactions12,13 or enhance cycling performance by producing LiPO2F2, a recognised electrolyte additive.14 Nevertheless, certain processing techniques, such as atomic layer deposition, are highly intricate and expensive, rendering them impractical for large-scale production.15
The layer-by-layer (LbL) methodology is an easily implementable and cost-effective method involving the amalgamation of nano-segments to cover diverse areas in various configurations.16 The LbL approach enables precise control of thickness at the nanoscale level. An exceptional feature of the LbL approach is its capacity to amalgamate organic and inorganic constituents for a thin film, integrating the attributes of each segment.16 The LbL process presents a promising avenue for attaining a uniform assembly of (1) materials within a narrow size range (100 nm to 1 μm), and (2) highly tailored composites.
Spray coating, as a LbL procedure, is both efficient and cost-effective for covering extensive areas. For example, spray coating may complete a 20-layer sample in about 4 min, but dip coating requires almost 2.5 h.17 Spray coating entails the application of a liquid substance onto surfaces by techniques such as air spray or electrostatic spray, facilitating uniform coverage and minimising the likelihood of drips and irregularities.18 This approach is adaptable, and suitable for a range of materials, including paints and specialised coatings. The application of the technique often utilises pressure devices that spray the coating, allowing small particles to cling well to intricate forms and surfaces. Spray coating offers superior regulation of thickness and texture, guaranteeing a uniform surface. Therefore, spray coating is extensively employed in the automotive, aerospace, and construction sectors, showcasing its versatility across diverse substrates and environments.19
This study involves the spray coating of graphite electrodes with alumina. Given its versatility and the ability to maintain consistent structure, composition, and thickness control, spray coating is proposed as a technique for electrode coating in batteries. The enhanced electrochemical performance of the as-prepared material is evidenced.
Component | Feature | Value |
---|---|---|
Graphite electrode | Areal capacity (mAh cm−2) | 0.807 |
Mass loading (mg cm−2) | 2.17 | |
Lithium metal | Thickness (μm) | 250 |
Current collector | Thickness (mm) | 0.010–0.012 |
Electrolyte | Composition | LP30 |
Electrolyte amount (drops) | 14 | |
Separator: glass fibre | Thickness (mm) | 0.556 |
Testing conditions | Testing temperature (°C) | 25 |
Minimum resting time (h) | 12 | |
Potential range (V) | 0.005–2 | |
Current density (mA cm−2) | 0.0807 |
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Fig. 1 (a) GDC curves of graphite anodes (cycles 1–4), (b) staging phenomenon (staging information from ref. 21), and (c) cycling performance of the raw material Al2O3 at 75 mA g−1. |
Fig. 1c illustrates that the electrode exhibits negligible capacity attributable to Al2O3, indicating that Al2O3 should be considered inert mass that does not enhance the specific capacity.
Coating powders directly is inadvisable because the insulating layer on the particles impedes the diffusion of Li+ ions and electron transport. Nonetheless, directly coating electrodes facilitates the establishment of a conductive pathway among particles. A uniform electrode surface coating is essential for attaining optimal electrochemical performance.8
Fig. 2a depicts an illustration of the coated electrode where substrate, electrode and coating are shown. Fig. S1 (ESI†) shows the SEM images of G0, G1, G4, and G7. No noticed variations among images are observed. Fig. 2b displays the XRD spectra of G0, G1, G4, G7, and Al2O3 powder. Fig. 2b is shown on this scale due to the remarkable intensity of the graphite (002) peak. No discernible alterations in the graphite crystal structure are seen in any of the four samples, suggesting that the spray coating process does not influence the crystal structure of the core material. The peaks at 36° and 67° correspond to Al2O3 (104) and (110), respectively.15 No significant difference in the XRD patterns of G4 and G7 is detected. Owing to the low mass ratio and amorphous characteristics of Al2O3, no discernible peaks of Al2O3 in the sample G1 can be seen.10
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Fig. 2 (a) Illustration of the obtained materials, and (b) XRD spectra of the samples and the raw Al2O3 powder. |
Fig. 3 illustrates the elemental mapping of carbon, aluminium, and oxygen in the as-prepared G1, G4, and G7 samples. It is demonstrated that all elements are detected when the weight proportion of components increases (G1 to G4). Nonetheless, a negligible signal in G7 may be affected by the coating bulk and electrical conductivity. Note that carbon mapping should be excluded as it is outside the purview of EDS.22
Fig. 4a illustrates the second-cycle GDC profile. As the mass ratio of Al2O3 coating increases, the specific charge capacity diminishes. The rationale for this is that the Al2O3 coating provides insufficient electrical conductivity, adversely affecting the specific capacity of lithium-ion batteries despite assertions of strong ionic conductivity.23 The initial coulombic efficiencies of the G0, G1, G4, and G7 are 81.5%, 82%, 82.3%, and 82.4%, respectively. The initial coulombic efficiency is positively related with the increases of the Al2O3 coating amount since Al2O3 coating may reduce excess lithium-ion consumption and inhibit adverse effects.10
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Fig. 4 (a) GDC curves for the second cycle at 0.1C within [0.005, 2] V, and (b) cycling stability of the samples at 0.1C within [0.005, 2] V. |
Fig. 4b illustrates the cycling stability of G1, G4, and G7 in comparison to G0 at 0.1C within [0.005, 2] V. G0, G1, G4, and G7 have specific charge capacities and capacity retention of 338 mAh g−1 (91.74%), 346 mAh g−1 (94.97%), 337 mAh g−1 (95.23%), and 290 mAh g−1 (85.29%), respectively. G1 and G4 exhibit superior capacity retention compared to G0, potentially attributable to the Al2O3 as the preformed SEI and the robust ionic conductivity derived from the stable Li–Al–O glass phase.23 Due to the limited performance of the G7, it is not considered in the following steps.
Fig. 5a illustrates the rate capacity of G0, G1, and G4 over different C-rates (0.1C–10C). It is demonstrated that when the C-rate surpasses 1C, G1 exhibits slightly better performance compared to G0 and G4. A slender layer with little ohmic polarisation yields a high specific capacity at low C-rates. However, at elevated C-rates, SEI regeneration leads to a comparatively diminished specific capacity.15 G1 operates at peak efficiency due to the coating functioning effectively as a preformed SEI, which reduces the loss of Li+ ions during SEI regeneration throughout cycling.
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Fig. 5 (a) Rate capacity at various C-rates (0.1C–10C) of G0, G1, and G4, and (b) EIS spectra of G0, G1, and G4. |
Fig. 5b displays the EIS spectra of G0, G1, and G4. Throughout the whole frequency spectrum, Nyquist plots exhibit three overlapping semicircles. The semicircles at high frequency correspond to the Rct of lithium-ion batteries. The low-frequency line pertains to the Zw. The Rct rises, moving from G0 (∼6.5 Ω), to G1 (∼7.5 Ω), to G4 (∼8.5 Ω) when the weight fraction of Al2O3 is increased.
A performance comparison between this study and existing literature is presented in Table 2. This work presents slightly better cycle retention. However, it is important to acknowledge that the electrochemical performance values are often not precisely comparable across different studies due to varying conditions, including fabrication methods, operational duration, binders, electrolytes, characterisations, and the limited information available. Standardisation initiatives have been undertaken within the battery sector,24–26 though no consensus has been reached yet.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ya00582a |
This journal is © The Royal Society of Chemistry 2025 |