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Large-scale direct regeneration of LiFePO4@C based on spray drying

Yongxing Zou ab, Jinwei Cao ab, Hao Li ab, Wanbao Wu ab, Yihong Liang ab and Jiaheng Zhang *ab
aSauvage Laboratory for Smart Materials, Harbin Institute of Technology (Shenzhen), Shenzhen, 518055, China. E-mail: zhangjiaheng@hit.edu.cn
bResearch Centre of Printed Flexible Electronics, School of Materials Science and Engineering, Harbin Institute of Technology (Shenzhen), Shenzhen, 518055, China

Received 21st July 2022 , Accepted 18th November 2022

First published on 13th December 2022


Abstract

Direct regeneration is a low-cost and environmentally friendly way of recycling spent Li-ion batteries. In this study, a new method is adopted to regenerate spent LiFePO4. First, the spent LiFePO4 powder is homogenized, and then, small amounts of a lithium source and a carbon source are thoroughly mixed by spray drying. After that, a high-temperature solid-phase method is used to regenerate the carbon-coated lithium iron phosphate. Compared with traditional regeneration methods, the proposed method significantly improves the universality of spent LiFePO4 having different degrees of damage. The regenerated LiFePO4 is characterized using X-ray diffraction, scanning electron microscopy, transmission electron microscopy, Raman spectroscopy, and electrochemical measurements. The results show that the regenerated sample has a stable morphology, structure, and electrochemical performance. Under the conditions of 0.1C, the initial capacity exceeds 160 mA h g−1. After 800 cycles under the conditions of 1C, the capacity retention is 80%, which satisfies the requirements for regenerated LiFePO4 batteries.

Keywords: LiFePO4; Direct regeneration; Homogenization; Spray drying; Electrochemical performance.


1 Introduction

Lithium-ion batteries (LIBs) are widely used in electronic devices owing to their high energy density and long service life. Among these, olivine lithium iron phosphate (LiFePO4 or LFP) has the advantages of thermal stability, long cycle life, and low cost, and it is popular for use in power batteries of electric vehicles.1 However, lithium-ion batteries have limited life spans. Generally, the life spans of these electric vehicle power batteries are 5–10 years. With the rapid development of electric vehicles, the next few years will usher in battery scrapping, which will inevitably generate a large number of end-of-life batteries.2,3 Recycling technology and harmless treatment technology for end-of-life batteries have become topics of concern.4–6

Research has focused on recycling valuable metals such as Co, Ni, and Li from cathode materials using various methods, such as hydrometallurgical technology, pyrometallurgical technology, and biotechnology.7–13 However, these processes are more suitable for waste LIBs containing the Ni and Co elements, such as LCO-, NCM-, and NCA-type, and are not applicable to waste LIBs without the Ni and Co elements, such as LFP- and LMO-type.14–16 Moreover, these recycling processes also have some obvious disadvantages: (a) the use of a large amount of chemical reagents, which is very likely to cause secondary pollution and generate a large amount of waste water and waste gas; (b) the process is long, and the cost of repair and regeneration is too high, thus compromising the practical application value.17–19 In contrast, direct regeneration of spent LFP is a more environmentally friendly method with practical application value.

Common regeneration methods are mainly hydrothermal and solid-phase regeneration.20–25 Hydrothermal regeneration mainly involves the repair of spent LFP by adding a specific proportion of a lithium source and a reducing agent. Xu et al.26 reported a low-temperature aqueous solution repair method for LiFePO4 using LiOH and citric acid as the lithium source and the reducing agent, respectively; the reaction was carried out at 60–180 °C for a certain time, followed by rapid annealing at 600 °C for 2 h. The electrochemical properties of the regenerated product were similar to those of commercial LiFePO4. Song et al.27 mixed LiFePO4 scraps with graphene oxide, added a lithium source and a reducing agent, and reduced graphene oxide while replenishing lithium in the hydrothermal liquid phase to obtain homogeneous and fine nanosphere composites. Solid-phase regeneration was mainly achieved by adding a lithium source (LiOH, Li2CO3) and a carbon source (glucose, lecithin, sucrose, and polyvinyl alcohol) to rehabilitate spent LFP by high-temperature roasting. Li et al.28 sintered recycled a cathode material with Li2CO3 and sucrose to regenerate new LiFePO4/C materials. The effect of Li2CO3 addition on the performance of the resynthesized LiFePO4/C material was investigated. The performance improved when the added amount of Li2CO3 was 1.4 wt%; the discharge capacity was 142.75 mA h g−1 in the first cycle at 0.2C conditions, and the retention rate was 95.32% after 100 cycles.

These repair and regeneration methods are helpful for the repair of spent LiFePO4; however, they have some shortcomings. The electrochemical properties of the regenerated samples under the same regeneration conditions can be inconsistent because the spent LiFePO4 could have been damaged to different degrees. This will limit the large-scale applications of the regenerated LiFePO4. Moreover, there are still some impurities in spent LiFePO4, such as residual electrolytes and binder, which hamper the formation of uniform and stable regenerated LiFePO4.29 The reported capacity values of the regenerated samples are relatively low, and it is challenging to achieve a comparable capacity to that of the unused LiFePO4.

To overcome the abovementioned challenges, we developed a closed-loop, scalable LIB recovery process that incorporates homogenization treatment, spray drying, and carbon thermal reduction (Fig. 1). The regenerated cathode material demonstrated excellent electrochemical performance, similar to that of commercial LiFePO4, especially under low rate conditions. The regeneration process is rapid, stable, and scalable. The specific process is as follows: (1) the spent lithium iron phosphate (S-LFP) battery cathode material was sintered at a high temperature in an air atmosphere to remove impurities and achieve homogenization; a red material primarily comprising Fe2O3 and Li3Fe2(PO4)3 was obtained. (2) The homogenized lithium iron phosphate (Homo-LFP) was mixed with Li2CO3 (lithium source), and ascorbic acid (reducing agent, carbon source) in deionized water. The mixed solution was placed in a ball mill and mixed thoroughly to obtain a spray-drying precursor solution. (3) The solution was spray-dried, and the resulting mixture was sintered in an Ar atmosphere, and a black powder was obtained. The black powder was rinsed with deionized water to remove water-soluble by-products; thus, carbon-coated lithium iron phosphate was obtained. The regenerated lithium iron phosphate (R-LFP) material exhibited excellent physical and electrochemical properties, and can meet the reuse requirements of commercial LFP batteries. This economical method has good application prospects.


image file: d2im00007e-f1.tif
Fig. 1 Schematic illustration of the regeneration process of spent LFP.

2 Results and discussion

2.1 Characterization of control and regenerated cathode materials

Inductively coupled plasma optical emission spectrometry (ICP-OES), and a carbon and sulfur analyzer were used to detect the elemental content of each sample. The major elemental compositions of S-LFP, Homo-LFP, and R-LFP are shown in Table 1. S-LFP contained approximately 4.41 wt% Li, 34.53 wt% Fe, 15.58 wt% P, and 1.38 wt% C. The molar ratio of Li[thin space (1/6-em)]:[thin space (1/6-em)]Fe is 1.02[thin space (1/6-em)]:[thin space (1/6-em)]1, which is slightly greater than 1. This could result from the over-discharge of the used battery before dismantling and some of the lithium-containing electrolytes remaining in the cathode powder. For R-LFP, approximately 4.47 wt% was Li, 31.29 wt% was Fe, 14.87 wt% was P, and 7.38 wt% was C. The molar ratio of Li[thin space (1/6-em)]:[thin space (1/6-em)]Fe[thin space (1/6-em)]:[thin space (1/6-em)]P was 1.09[thin space (1/6-em)]:[thin space (1/6-em)]1[thin space (1/6-em)]:[thin space (1/6-em)]0.98. A small amount of lithium source was added to ensure that lithium is correctly positioned in the regenerated LFP and to reduce Li–Fe “anti-site” pairs.30 The regeneration process increases the Li–Fe ratio from 1.02 to 1.09 and the carbon content from 1.31 to 7.38 wt%, which facilitates the reduction of Li–Fe anti-sites and achieves carbon encapsulation of LFP.
Table 1 The major element content of the samples
Mass ratio/% Fe Li P C
S-LFP 34.53% 4.41% 15.58% 1.31%
Homo-LFP 31.29% 4.47% 16.38% ∼0
R-LFP 27.39% 3.74% 14.87% 7.38%


The crystalline structure of S-LFP was analyzed by X-ray diffraction (XRD), as shown in Fig. 2a. Though the diffraction peaks of the discarded S-LFP powder are dominated by olivine LFP (JCPDS 81-1173), the impurity peaks near 2θ = 22.3° and 2θ = 23° are non-negligible. Fig. 2b shows the XRD patterns of Homo-LFP and R-LFP. The homogenized sample mainly comprised Fe2O3 (JCPDS 89-0597) and Li3Fe2(PO4)3 (JCPDS 47-0107). The XRD spectrum of R-LFP was in good agreement with the standard PDF card (#81-1173, LiFePO4). The diffraction peaks are sharp and clear, and no other phases or impurities can be observed, which indicates that the regeneration process could effectively restore the crystalline structure of LFP.


image file: d2im00007e-f2.tif
Fig. 2 Phase analysis and morphological characterization of samples. XRD patterns of (a) S-LFP, (b) Homo-LFP and R-LFP; SEM images of (c) S-LFP, (d) Homo-LFP, (e) spray-dried LFP and (f) R-LFP; (g and h) TEM images of R-LFP; (i and j) HAADF-STEM image and EDS elemental mappings of R-LFP.

Fig. 2c shows the scanning electron microscopy (SEM) images of spent LiFePO4. The morphology of the spent sample was irregular, showing more agglomerates and even a tiny amount of incompletely decomposed PVDF binder. The agglomerates and residual PVDF could hinder Li+ transport during charging and discharging, which would reduce the electrochemical performance.31Fig. 2d shows the SEM images of samples after the homogenization treatment, where the large agglomerates disappeared and the PVDF binder was eliminated. Fig. 2e shows the microscopic morphology after spray drying, and it can be observed that the secondary particles exhibited hollow-sphere-like structures. Fig. 2f shows the microscopic morphology of the R-LFP sample, which maintains a hollow spherical shell secondary structure.

High-resolution TEM (HR-TEM) was used to observe the morphologies of the regenerated sample. Fig. 2g and h show that the microstructure of R-LFP was regular with high crystallinity, and the measured layer spacing was 0.348 nm, which corresponded to the (111) crystal plane of LiFePO4. A coating layer of 3 nm can be observed at the particle surface, which is attributed to a layer of carbon coating. Carbon coating on the surface helps to improve the electrochemical properties and prevent excessive grain growth. Fig. 2i shows the HAADF-STEM image of R-LFP, where elliptical grains with a long axis of approximately 110.5 nm can be distinguished. The energy dispersive X-ray spectroscopy (EDXS) mappings of the main elements C, Fe, and P for R-LFP are shown in Fig. 2j, which indicates the uniform element distribution throughout the sample.

Surface analysis of S-LFP, Homo-LFP, and R-LFP was carried out using X-ray photoelectron spectroscopy (XPS). As shown in Fig. 3a, the XPS survey spectra of S-LFP, Homo-LFP, and R-LFP clearly show the elemental peaks of P 2s, C 1s, O 1s, and Fe 2p. The calibration of all the sample peaks was conducted with respect to the C 1s species. In S-LFP and R-LFP, the signal of C 1s is deconvoluted into three peaks, at binding energies of 284.8 eV (C–C), 286 eV (C–O–C), and 288.5 eV (O–C[double bond, length as m-dash]O).32 The distribution of the types of C species in the samples is illustrated in Fig. 3b. The ratio of C–O–C to C–C in S-LFP could be determined from the XPS result, which is 0.44. On the other hand, in R-LFP, this ratio is 0.21, which shows that R-LFP has fewer defects in the carbon layer. Similarly, the signal of Fe 2p is deconvoluted into four peaks.33 The distribution of Fe in the samples is illustrated in Fig. 3c. XPS revealed that the ratio of Fe3+ to Fe2+ was 0.67 in S-LFP and 0.53 in R-LFP, indicating that there were fewer Fe3+ impurities in the regenerated samples.


image file: d2im00007e-f3.tif
Fig. 3 XPS and Raman spectra of the samples. (a) XPS survey spectra for the samples; high-resolution spectra of (b) C 1s and (c) Fe 2p; (d) Raman spectra of the samples.

The presence of carbon in the samples was further characterized by Raman spectroscopy. The Raman spectra of the samples are listed in Table 2. D-band and G-band peaks were observed at ∼1360 cm−1 and ∼1560 cm−1, respectively, representing the lattice defects and the in-plane stretching vibration of the sp2 hybridized C atoms.34 Comparing the ID/IG (intensity ratio of the D-band to the G-band) of the samples, it is observed that the ID/IG of the regenerated samples is much smaller than that of the spent LFP. This indicates a higher degree of graphitization of the carbon cladding layer in the regenerated LFP. The higher degree of graphitization is beneficial to improve the electrical conductivity and thus to improve the charge/discharge performance of the regenerated samples. The absence of the D-band and G-band in the homogenized LFP indicated that the residual carbon in the spent LFP was sufficiently removed, and the regenerated sample was not affected by the residual PVDF and organic electrolyte, which significantly improves the stability of the regeneration.

Table 2 Raman data of the samples
Sample I D I G I D/IG
S-LFP 8579.22 6106.80 1.4049
Homo-LFP No peak No peak
R-LFP 10[thin space (1/6-em)]938.50 9818.90 1.1140


2.2 Electrochemical performances of spent and regenerated LiFePO4

The first four cycles of voltammetry results for the spent and regenerated LFP are shown in Fig. 4a and b, respectively. They comprise a pair of anode and cathode peaks, representing the charge–discharge reaction. The regenerated LFP had a small potential difference (0.292 V) between the two redox reactions, which was significantly smaller than that of the spent LFP (0.352 V). This indicates that the cell containing regenerated LFP had a lower polarization. In the subsequent cycles, the peak position and the intensity of R-LFP remained stable, which indicates the high reversibility of the regenerated sample. This suggests that the cyclic performance of the regenerated sample was much better than that of the spent LFP.
image file: d2im00007e-f4.tif
Fig. 4 Electrochemical performances of S-LFP and R-LFP. CV curves of (a) S-LFP and (b) R-LFP; (c) Nyquist plots of R-LFP and S-LFP; charge–discharge curves of (d) S-LFP and (e) R-LFP at different rates; (f) rate performance of samples; (g) long-term cycling stability of S-LFP and R-LFP; (h) charge–discharge curves of R-LFP after several cycles.

To further understand the electrochemical performance of the regenerated samples, EIS measurements were performed in the frequency range of 100 kHz–0.05 Hz with an uptake amplitude of 10 mV. Fig. 4c shows the Nyquist plots of the spent and regenerated LFP samples. The EIS spectrum comprised a depressed semicircle in the high-frequency region and a straight line in the low-frequency region. In general, the total resistance (Rs) of the electrolyte and electrode material was the intercept of the semicircle in the high-frequency region, and the charge-transfer resistance (Rct) was the semicircle diameter.35 The corresponding Rs and Rct values (as listed in Table 3) could be obtained by fitting the EIS curves with an equivalent circuit model. Table 3 shows that the regenerated sample had smaller Rs and Rct values. The results indicate that the EIS performance of the regenerated sample was superior because of the improved particle structure, good carbon encapsulation, and low impurity content.36

Table 3 Equivalent circuit parameter fitting based on experimental data
Sample R s (Ω) R ct (Ω)
Spent LFP 4.378 131.7
Regenerated LFP 1.866 81.61


The charging and discharging curves of spent LFP and regenerated LFP at different rates are shown in Fig. 4d and e; the discharge capacities of S-LFP were 124.6, 114.2, 100.7, 86.8, and 70.0 mA h g−1 at discharge rates of 0.1, 0.2, 0.5, 1, and 2C, respectively. Meanwhile, the discharge capacities of R-LFP were 160.8, 150.0, 130.6, 117.3, and 100.1 mA h g−1 at discharge rates of 0.1, 0.2, 0.5, 1, and 2C, respectively. The charge/discharge specific capacity of the regenerated LiFePO4 was better than that of the spent LiFePO4 sample.

As shown in Fig. 4f, the rate performance of each sample exhibited a clear stepwise trend. The discharge capacities of the regenerated LFP at 0.1, 0.2, 0.5, 1, and 2C were ∼160, ∼150, ∼135, ∼120, and ∼100 mA h g−1, respectively, which are much better than those of the spent LFP. The cycling performance of the regenerated LiFePO4 and spent LiFePO4 at 1C rate is shown in Fig. 4g. After 600 cycles, the discharge performance of the spent LFP decreased significantly. The regenerated LFP maintained approximately 80% capacity after 800 cycles, and the coulombic efficiency was steadily maintained near 100%. The charging and discharging curves of R-LFP after several cycles are shown in Fig. 4h, and the voltage of the charging and the discharging platform remains stable during the cycle. The discharge capacities of the regenerated LFP at the 1st, 5th, 10th, 50th, 100th, 500th, and 800th turns were 115.1, 112.9, 111.8, 110.3, 115.7, 92.2, and 87.9 mA h g−1, respectively. The regenerated LiFePO4 exhibited excellent cycling performance and was capable of meeting industrial recycling requirements.

In addition, the regeneration of 1 ton lithium iron phosphate by this method requires 1 ton of S-LFP black powder, 0.01 tons of lithium carbonate, and 0.07 tons of glucose. The cost of these materials is ¥72[thin space (1/6-em)]339 per ton, which is 51.02% that of the raw material lithium iron phosphate (please see the ESI for assessment details). The cost of regeneration is significantly lower than the market price of lithium iron phosphate and provides a basis for industrial production.

3 Conclusion

In this study, a scalable and closed-loop lithium-ion battery recycling process is proposed. The process includes homogenization, spray drying, and carbon thermal reduction. Regenerated LiFePO4@C shows a restored lattice structure, uniform surface carbon coating, and excellent electrochemical properties. In this work, the regenerated LiFePO4 shows a capacity of more than 160 mA h g−1 at 0.1 C and maintained approximately 80% of the initial capacity value at a 1C rate for 800 cycles. The regenerated LiFePO4 had stable performance, and the regeneration method was simple and resource-saving, showing great potential for application to the recycling industry.

4 Experimental procedures

4.1 Sample preparation

Spent LFP was provided in large quantities by a local professional power battery recycling company (Shenzhen Hengchuang Ruineng Environmental Technology Co. Ltd.). Super P, polyvinylidene fluoride (PVDF), N-methylpyrrolidone (NMP), LiPF6, dimethyl carbonate (DMC), and ethylene carbonate (EC) were provided by Guangdong Canrd New Energy Technology Co., Ltd.

To remove impurities in the spent LFP powder and homogenize the composition, 50 g of spent LFP was weighed into a porcelain boat and placed in a muffle furnace at 800 °C for 150 min. This step helps to sufficiently remove the remaining electrolyte, adhesive, carbon black, and other impurities.

4.2 Spray drying and sintering to obtain regenerated LFP

The process mainly consists of precursor preparation, spray drying, and roasting. An appropriate amount of the sample was taken after the aforementioned treatment to prepare an aqueous solution. Li2CO3 (1 wt%), ascorbic acid (30 wt%), a small amount of graphene, and sodium dodecylbenzene sulfonate were added as surfactants, and all the components were mixed thoroughly by wet ball milling. In this experiment, 10 g of lithium iron phosphate, 0.1 g of Li2CO3, 3 g of ascorbic acid, and 0.1 g of sodium dodecylbenzene sulfonate were mixed in 100 mL of deionized water, and then wet ball milled at 280 rpm for 10 h. After spray drying of the precursor solution, 4 g of the spray-dried product was placed in a porcelain boat and roasted at 350 °C for 4 h under an atmosphere containing Ar to obtain a black powder; then, this powder was heated to 650 °C for 10 h at a rate of 3 °C min−1. The black powder was rinsed with deionized water to remove water-soluble by-products and dried under vacuum at 80 °C for 24 h to obtain the carbon-coated LFP.

4.3 Characterization of the composition and structure of the sample

The elemental composition of the sample was determined using inductively coupled plasma optical emission spectrometry (ICP-OES, Agilent 720ES). The phase composition was determined using X-ray diffraction (XRD, Rigaku Ultima VI Type), and the morphology was examined using scanning electron microscopy (SEM, Zeiss Sigma300). X-ray photoelectron spectroscopy (XPS, KRATOS AXIS Ultra DLD) was used to characterize the valence states of Fe and C on the sample surface. Raman spectroscopy (Horiba Scientific LabRAM HR Evolution) was used to characterize the carbon coatings on the surfaces. Transmission electron microscopy (TEM, FEI Talos F200X) was used to observe the thickness of the carbon coating and the lattice spacings.

4.4 Electrochemical performance of regenerated LFP

The cathode was prepared by coating a slurry containing 80% active material, 10% Super P, and 10% PVDF. After the addition of NMP, the slurry was stirred for 12 h. The slurry was coated on an aluminum foil substrate and then vacuum-dried at 80 °C for 12 h.

The amount of active material was approximately 1.5 mg cm−2. Electrochemical measurements were performed at 25 °C using a CR2032 coin-type battery with lithium as the anode. A DMC–EC mixed solvent containing 1.0 M LiPF6 and 5% FEC was used as the electrolyte. The battery was assembled in a glove box filled with argon, and the H2O and O2 contents were <0.1 ppm. A Neware instrument was used to study the constant current charge and discharge capacity and rate performance at different current densities in the voltage range of 2.5–4.2 V. Cyclic voltammetry (CV) tests were performed on a CHI 760E (CH, Shanghai, China) electrochemical workstation with voltages of 2.5 and 4.2 V, and a scan rate of 0.01 mV s−1. For electrochemical impedance spectroscopy (EIS), the frequency range was selected from 100 kHz to 0.05 Hz, and the amplitude was 10 mV.

Conflicts of interest

The authors declare no conflict of interest.

Acknowledgements

This work was supported by the National Natural Science Foundation of China (21703218 and U21A20307), the Shenzhen Science and Technology Innovation Committee (JCYJ20180507183907224 and KQTD20170809110344233) and the Guangdong Province Covid-19 Pandemic Control Research Fund (2020KZDZX1220).

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Footnote

Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2im00007e

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