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JOM

, Volume 71, Issue 12, pp 4473–4482 | Cite as

Sulfation Roasting Mechanism for Spent Lithium-Ion Battery Metal Oxides Under SO2-O2-Ar Atmosphere

  • Junjie Shi
  • Chao PengEmail author
  • Min Chen
  • Yun Li
  • Hurman Eric
  • Lassi Klemettinen
  • Mari Lundström
  • Pekka Taskinen
  • Ari JokilaaksoEmail author
Open Access
Extraction and Recycling of Battery Materials
  • 300 Downloads

Abstract

Sulfation roasting followed by water leaching has been proposed as an alternative route for recycling valuable metals from spent lithium-ion batteries (LIBs). In the present work, the reaction mechanism of the sulfation roasting of synthetic LiCoO2 was investigated by both thermodynamic calculations and roasting experiments under flowing 10% SO2-1% O2-89% Ar gas atmosphere at 700°C. The products and microstructural evolution processes were characterized by x-ray diffraction, scanning electron microscope and energy dispersive x-ray spectrometer, and atomic absorption spectroscopy. It was confirmed that Co3O4 was formed as an intermedia product, and the final roasted products were composed by Li2SO4, Li2Co(SO4)2, and CoO. The leaching results indicated that 99.5% Li and 17.4% Co could be recovered into water after 120 min of roasting. The present results will provide the basis and solid guidelines for recycling of Li and Co from spent LIBs.

Introduction

The circular economy has become a hot topic worldwide during recent years. It requires the circulation of materials and energy, especially recycling from secondary resources.1 During the last 20 years, a huge amount of spent lithium-ion batteries (LIBs) has been generated as a result of the increasing consumption of LIBs since their commercialization by SONY Inc. in 1991.2 The amount of battery waste will increase exponentially as the batteries of electric vehicles (EV) come into end of life. In 2017, nearly 1.1 million EVs were sold worldwide, whereas in 2025 the amount will be ca. 11 million. Consequently, the predicted global amounts of battery metals ending up in recycling in 2035 will be ca. 104 GWh (with 8 years first life and 5 years second life for 70% of batteries), corresponding to ca. 7.5 kt Li and 12 kt Co.3,4

Spent LIBs can be treated as valuable secondary sources of metals because of their large amounts of Li, Co, Ni, Mn, Cu, Al, and Fe,5,6 which are present in higher concentration than in natural primary ores.7 Typically, a spent Li-ion battery contains 5–20 wt.% Co, 5–7 wt.% Li, 5–7 wt.% Ni, 15 wt.% organics, and 7 wt.% plastics.8 However, only about 5% of spent portable LIBs are recycled today, and LIB production will suffer a global supply shortage of key elements including Li, Co, and Ni due to the increasing demand for consumer electronic devices and EVs.9 On the other hand, if the spent LIBs are not treated properly, they will cause serious environmental pollution such as soil and groundwater contamination by the leakage of electrolytes such as lithium hexafluorophosphate (LiPF6) if they are burned or exposed to air or water.10,11 Therefore, the recycling of spent LIBs is necessary to alleviate the unprecedented demand for raw materials for the synthesis of LIBs as well as environmental and economic benefits.

Currently, the worldwide spent LIB recycling technologies can be classified into hydrometallurgy, pyrometallurgy, or their combination.9,12 In the hydrometallurgical processes, the spent LIBs first need to be pretreated to enrich the target metals, e.g., by discharging, dismantling, crushing, etc.,13, 14, 15 and then dissolved into inorganic acids or organic acids.16, 17, 18, 19, 20, 21 The resultant Co, Li-rich acidic leaching solution is then subjected to the subsequent purification and recovery process, for instance, chemical precipitation,22 solvent extraction,23 or ion-exchange24 methods. Nonetheless, these hydrometallurgy technologies involve high levels of chemical consumption, weak adaptability to input materials, and high risk of fire or explosion during the discharging process.25 In contrast, pyrometallurgical technology such as smelting does not need an additional discharging process and exhibits strong adaptability to input materials. The high-temperature smelting process has been industrially utilized by various companies (e.g., Toxco Inc., USA; Sony Corp., France), through which Co and Ni can be recovered as alloys, whereas the majority of Li is ready to end up within the slag fraction and dusts.26, 27, 28

Considering the abovementioned shortcomings of the hydrometallurgy and pyrometallurgy methods, researchers are starting to look for combined methods to treat LIBs waste, e.g., by nitration roasting,18 sulfation roasting,29 reduction roasting with carbon,30 or vacuum evaporation31 followed by water leaching. Among these methods, sulfation roasting-water leaching is considered one of the most promising as this process has been extensively investigated for the extraction of valuable metals such as Cu, Ni, Co, V, and Mn from different primary and secondary ores including pyrite, nickel sulfide ore, copper concentrate, and lepidolite.32, 33, 34, 35 The core concept of this method is to selectively transfer the desired metals (e.g., Co and Li) into soluble sulfates, but leave the other unwanted impurities as insoluble oxides. A recent study by Wang et al.36 revealed that Li could be selectively extracted from spent LIBs via an indirect sulfation roasting process with the SO3 gas generated by the decomposition of NaHSO4·H2O. However, the mechanism of the sulfation roasting process is still unclear, and more efforts are needed to fully understand it.

In the present work, sulfation roasting followed by water leaching is proposed for the recycling of spent LIBs, and the reaction mechanism under SO2-O2 atmosphere will be elaborated from both the thermodynamic and experimental aspects. The novelty of this process is not only an alternative method for handling spent LIBs, their lithium, and base metals, but also an option for recovering rare earth elements such as sulfates.37

Materials and Methods

Materials

To clarify the recycling mechanism of active materials present in spent LIBs under SO2-O2 atmosphere, synthetic LiCoO2 powder with a purity of ≥ 97 wt.% (Alfa Aesar, Germany) was selected as a compound representing the typical cobalt-rich component of spent LIBs. LiCoO2 powder was first dried at 120°C for 24 h to evaporate the water and other volatiles. For each experiment, an initial amount of 4.00 g (m0) LiCoO2 powder was weighed (by 0.0001 g balance) and uniformly distributed in the silica crucible (130 mm long, 30 mm wide, 9.5 mm high, 3.5 mm thick) for further steps.

Sulfation Roasting Experiments

Sulfation roasting experiments were carried out in a horizontal tube furnace (Fig. 1). The silica crucible containing LiCoO2 powder was slowly pushed into the hot zone, and the temperature was measured by a K-type thermocouple and controlled by a Keithley 2000 multimeter intelligent temperature controller (accuracy of ± 1°C, Tektronix, Inc., Beaverton, OR, USA). After the temperature of the crucible reached the target value, a pre-roasting experiment was first conducted for sample S1 under 400 mL/min Ar (99.999%, AGA, Finland) atmosphere. Thereafter, samples S2 to S12 were employed to be roasted under SO2-O2-Ar gas mixture with a total flow rate of 400 mL/min. The gas composition was achieved by mixing SO2 (99.99%) and O2 (99.99%) with Ar (99.999%) (AGA, Finland). The flow rates of these gases were controlled by DFC digital mass flow meters (Aalborg, USA). The offgas was cleaned by NaOH solution with BTS as an indicator (bromothymol blue, C27H28Br2O5S, Sigma-Aldrich, USA) to remove SO2 before venting to the fume hood.
Fig. 1

Schematic of the sulfation roasting experimental setup

After the preset roasting time, the silica crucible was quickly removed from the furnace and cooled in air. The reacted product after sulfation roasting (m1) was accurately weighed to calculate the weight increase ∆m (∆m =m1m0, g) and relative weight increase α (α = ∆m/m0, %).

Analytical Methods

The roasted products were leached with water at 25°C for 60 min to produce a leachate and leach residues under the conditions of a solid/liquid ratio of 100 g/L. After the leaching step, the leachate was separated by centrifugation at 4000 rpm for 10 min (S/L) at room temperature. The leach residue was then fully digested by nitrohydrochloric acid to analyze the chemical composition. After proper dilution, solutions from the leachate and residue were analyzed by atomic absorption spectroscopy (AAS, Varian AA240, Agilent Technologies, CA, USA) to determine the concentrations of Li and Co.

The roasted samples and leach residues were characterized by x-ray diffraction (XRD, PANalytical X’Pert Pro Powder, Almelo, The Netherlands) using Co Kα radiation at a scan rate of 2°/min from 15° to 90° (acceleration potential 40 kV, current 30 mA). Quantitative phase composition of the XRD results was performed by HighScore Plus 4.1 software (PANalytical) using Rietveld fitting, based upon the PDF2 powder database.38 Meanwhile, the microstructures of phases were analyzed using a Tescan MIRA 3 scanning electron microscope (SEM, Tescan, Brno, Czech Republic) equipped with an UltraDry Silicon Drift energy-dispersive x-ray spectrometer and NSS microanalysis software (EDS, Thermo Fisher Scientific, Waltham, MA, USA). An accelerating voltage of 5 kV and beam current of 10 nA were employed for the SEM analysis, while for the EDS detection, an accelerating voltage of 15 kV and a beam current of 20 nA were used. Proza (Phi–Rho–Z) matrix correction procedure39 was employed for raw data processing, and the standards utilized in EDS analyses were metal Co (for Co, Lα), quartz (for O, Kα), and marcasite (for S, Kα).

Thermodynamic Calculations

Nowadays, commercial thermodynamic software such as HSC40 has been developed to make predictions of complex reactions for oxide and sulfide systems. In the present work, HSC Chemistry 941 was employed to calculate the equilibrium assemblages for the Li-Co-S-O system.

Results and Analysis

Thermodynamics

The formation of sulfate can be described by the reactions of oxide in SO2-O2 gas mixtures or SO3 gas atmosphere, as shown in Eqs. 1, 2, and 3.
$$ {\text{MO}}_{x} \left( {\text{s}} \right) \, + \, 0.5x\;{\text{O}}_{2} \left( {\text{g}} \right) \, + x{\text{SO}}_{2} \left( {\text{g}} \right) \, = {\text{ M}}\left( {{\text{SO}}_{4} } \right)_{x} \left( {\text{s}} \right) $$
(1)
$$ 2{\text{SO}}_{2} \left( {\text{g}} \right) \, + {\text{ O}}_{2} \left( {\text{g}} \right) \, = \, 2{\text{SO}}_{3} \left( {\text{g}} \right) $$
(2)
$$ {\text{MO}}_{x} \left( {\text{s}} \right) \, + x{\text{SO}}_{3} \left( {\text{g}} \right) \, = {\text{ M}}\left( {{\text{SO}}_{4} } \right)_{x} \left( {\text{s}} \right) $$
(3)
Therefore, the stability of the sulfates of interest was calculated by HSC and is shown in Fig. 2 as the predominance area diagram of the Li-Co-O-S system, at temperatures from 600°C to 800°C. It is clear that Li2SO4 is stable at higher SO2 and O2 partial pressures from 600°C to 800°C, while Co may exist as CoO, Co3O4, and CoSO4 in different O2 and SO2 partial pressures. Accordingly, the predominance area diagram could also be divided into five phase combination domains at a fixed temperature, i.e., Li2SO4 + CoSO4, Li2SO4 + CoO, Li2SO4 + Co3O4, Li2O + CoO, and Li2O + Co3O4. This means that a selective sulfation or co-sulfation roasting can be achieved by adjusting the operational point in the roaster. As a result, the experimental condition with an atmosphere of 10% SO2 and 1% O2 at 700°C (point A in Fig. 2) was selected for the sulfation roasting experiments to explore the reaction mechanism.
Fig. 2

Predominance area diagram obtained by superimposing Li-S-O and Co-S-O diagrams from 600°C to 800°C

Macrophotograph and Weight Difference

The macrographs after sulfation roasting experiments under a 10% SO2-1% O2-89% Ar atmosphere at 700°C, as well as the weight differences (weight increase ∆m and relative weight increase α) and the conversion ratios, are presented in detail in Fig. 3. Before the sulfation roasting experiment, a roasting pre-experiment was carried out for sample S1 under 400 mL/min Ar atmosphere at 700°C with 180 min. Both the macrophotograph in Fig. 3a and the weight difference in Fig. 3b indicate that there was no reaction during the process, and sample S1 still presented the original powder state compared with the raw material.
Fig. 3

Macrograph of color evolution, weight change (∆m and α), and conversion during sulfation roasting at 700°C. (a) Macrographs; (b) ∆m and α; (c) conversion ratio, β

For samples S2 to S9, the color change in Fig. 3a clearly suggested that the sulfation roasting reaction continuously proceeded with time, extending from 2 min to 60 min. A light-yellow color could be observed at the left corner of sample S3 when the roasting time was increased to 5 min, while the other parts of sample S3 still kept the original color compared with the raw LiCoO2 powder. Thereafter, the color changed gradually from the left to right side along with the gas flow direction when the time was increased from 5 min to 25 min, and only a small part at the right corner of the sample kept the original color at 25 min. When the time was further increased to 60 min, the entire sample turned light yellow, as demonstrated by sample S9 in Fig. 3a. It is worth mentioning that the sulfation roasting reaction was also characterized by the densification of the products, which means neck growth between the product particles.

The color change of the roasted samples was also accompanied by weight changes, characterized by weight increase ∆m and relative weight increase α in Fig. 3b. Figure 3b shows that the relative weight was rapidly increased from 3% at 2 min to 44% at 30 min. Thereafter, there was only a small weight increase even if the roasting time was increased to 240 min, which implies that most of the sulfation reactions were completed during the first 30 min. According to the experimental atmosphere of point A in Fig. 2, the final roasted products should be a blend of Li2SO4 + CoSO4. This means the conversion β should reach close to 100% when the time is extended beyond 30 min. However, an interesting result is discovered when conversion β along with time is plotted with reference to the final roasted products of Li2SO4 + CoSO4; this is shown in Fig. 3c with the black squares. The highest conversion only can reach 44%, even for 240 min, and this inconsistency implies some other phases must be formed during roasting. To solve this confusion, a simple assumption with the final products of Li2SO4 + CoO or Li2SO4 + Co3O4 was used to calculate the conversion for comparison in Fig. 3c. Conversions > 100% were observed after 25 min for both assumptions, which indicates the final products were not simple combinations of Li2SO4 + CoO or Li2SO4 + Co3O4.

Phase Evolution During Sulfation Roasting Reactions

The existing phases and corresponding microstructures after sulfation roasting were characterized by XRD and SEM–EDS, as shown in detail in Fig. 4a, b, and c, respectively.
Fig. 4

Phase evolution and the corresponding microstructures characterized by XRD and SEM–EDS. (a) XRD patterns for the raw LiCoO2 powder of samples S4 and S9 after sulfation roasting. (b) Microstructures for samples S4 and S9 after sulfation roasting; (c) XRD patterns for samples roasted from 2 min to 240 min at 700°C

As observed in Fig. 3a, sulfation roasting gradually took place from the left to right side along with the gas flow direction, resulting in faster reactions on the left side than the right side of the crucible. Therefore, sample S4 reacted for 10 min and sample S9 reacted for 60 min were taken as examples to explore the phase assemblies during roasting. Sample S4 was divided into three sections and labeled as left, center, and right along with the gas flow direction, as shown in Fig. 4a. Compared with the XRD patterns of raw LiCoO2 powder, Li2SO4, Co3O4, and a small amount of CoO started to emerge in the right section of sample S4. In the center section of S4, binary sulfate of Li2Co(SO4)2 was formed. Meanwhile, the relative intensities of Li2SO4, Co3O4, and CoO became stronger, while the intensity of LiCoO2 got weaker, which indicated development of an increasing fraction of Li2SO4, Co3O4, and CoO. Furthermore, in the left section of sample S4, it could be found that the relative intensities of Li2SO4, Li2Co(SO4)2, and CoO increased, while the intensities of LiCoO2 and Co3O4 phase decreased. Thus, Co3O4 was first produced as an intermediate product and consumed thereafter. The corresponding SEM microstructures for sample S4 are shown in Fig. 4b. Many small particles were observed on the surfaces of a bigger matrix when the roasting reaction proceeded from the right to the left section.

In Fig. 4a, more complete sulfation roasting results are demonstrated by sample S9. The XRD patterns of S9 showed that when increasing the roasting time to 60 min, there was no LiCoO2 left, and the final products were Li2SO4, Li2Co(SO4)2, CoO, and a small amount of Co3O4. This is consistent with the trends of the results in sample S4. The microstructure for sample S9 in Fig. 4b also showed many small particles. However, an obvious difference was also observed in the phase matrix. Signs of melting compared with the particles in sample S4 were observed, and the EDS results indicated the matrix as the sulfate, while the particles were mostly CoO, as shown in Fig. 4b.

In Fig. 4c, XRD patterns for samples roasted in 10% SO2-1% O2-89% Ar gas from 2 min to 240 min are plotted together for comparison. It can be concluded that with proceeding roasting reactions, the intensity of LiCoO2 (20°–25°) kept decreasing until the peaks fully disappeared. At the same time, the intensities of Li2Co(SO4)2 (17°–20°) and Li2SO4 (25°–27°) became increasingly strong. However, the XRD patterns between 40° and 45° indicate that the intensity of Co3O4 was first increased and then decreased. The intensity of CoO (40°–45°) also became stronger, implying a spontaneous transformation from Co3O4 to CoO. The XRD patterns from 40° to 45° also showed the intensity of LiCoO2 phase faded away. Therefore, the final products after sulfation roasting were confirmed as Li2SO4, Li2Co(SO4), and CoO, and this explains why the conversion β in Fig. 3b was much lower with the assumption of Li2SO4 + CoSO4 as the final product or much higher with the assumption of Li2SO4 + CoO and Li2SO4 + Co3O4.

Water Leaching

The samples after sulfation roasting experiments were exposed to water leaching at 25°C for 60 min. The leaching results are shown in Fig. 5a and b, respectively. As Fig. 5a shows, the leaching yield of Li significantly increased from 6% at 2 min to 99% at 30 min, and 99.5% Li was finally recovered in water when the roasting time increased to 120 min. In contrast, the leaching efficiency of the cobalt element increased slowly, and only 17.4% Co was leached even after a roasting time of 120 min.
Fig. 5

Water leaching results. (a) Leaching efficiency for sulfation roasted samples from 2 min to 120 min, %; (b) XRD patterns and microstructures for leaching residues of samples S4 and S9; (c) different phases presented in leaching residues, %

The XRD patterns of roasted sample S4 and S9 in Fig. 5b showed that only the oxides were left in the leaching residue, which means that the sulfates of Li2SO4 and Li2Co(SO4)2 were leached by water. The corresponding SEM microstructures in Fig. 5b were demonstrated mainly as small particle phases, consistent with the microstructures found in Fig. 4b, indicating that the matrix phase was dissolved in water. Furthermore, the quantitative calculation based on the intensities42 of the phases indicated that the unreacted LiCoO2 in the leaching residue dropped from 91% at 2 min to only 0.7% at 25 min, as shown in Fig. 5c. At the same time, the content of Co3O4 in residue was first increased to 21% at 10 min and then decreased to 1% at 25 min. Meanwhile, the CoO content continuously increased to 99.3% at 60 min; this result is consistent with the XRD results for sample S4 in Fig. 4a.

Mechanism of the Sulfation Roasting Reaction

A significant discrepancy was found between the predicted and experimental result, as the calculated CoSO4 phase was not detected during sulfation roasting, while the detected Li2Co(SO4)2 phase was not considered in the calculations by HSC. The Li2SO4-CoSO4 binary phase diagram43, 44, 45 confirmed that Li2Co(SO4)2 phase is a double sulfate with an incongruent melting temperature of 610°C. The reason why Li2Co(SO4)2 was identified in the present experimental conditions must be that Li2Co(SO4)2 becomes more stable in the higher partial pressure of a SO2 atmosphere compared with the Ar gas used for the determination of the Li2SO4-CoSO4 binary phase diagram.43, 44, 45 However, the thermodynamic data of Li2Co(SO4)2 were not available in the HSC software database.

Based on the end products and discussions above, the sulfation roasting reaction under 10% SO2-1% O2-89% Ar gas mixture at 700°C can be described by the overall reaction R1. The roasting mechanism can be further subdivided into three stages, as shown in Fig. 6.
$$ \text{Overall reaction:}\,4{\text{LiCoO}}_{2} \left( {\text{s}} \right) \, + \, 3{\text{SO}}_{2} \left( {\text{g}} \right) \, + {\text{ O}}_{2} \left( {\text{g}} \right) \, = {\text{ Li}}_{ 2} {\text{SO}}_{4} \left( {\text{s}} \right) \, + {\text{ Li}}_{ 2} {\text{Co}}\left( {{\text{SO}}_{4} } \right)_{2} \left( {\text{s}} \right) \, + \, 3{\text{CoO }}\left( {\text{s}} \right)\quad (R1) $$
Fig. 6

Mechanism of sulfation roasting process under 10% SO2-1% O2-89% Ar gas at 700°C

The first stage was mainly related to the production of Co3O4 and Li2SO4, and the related reactions in stage 1 are shown as (R2) to (R6). According to the relationship of ∆Gθ (kJ mol−1) with temperature (°C) calculated by HSC in Fig. 7a, LiCoO2 would not decompose to oxides by reactions (R2) and (R3) at 700°C. SO3 was produced by reaction (R4), which made it feasible to transform LiCoO2 to Li2SO4 and Co3O4 by both the sulfation roasting reactions in SO2-O2 gas mixture [reaction (R5)] and SO3 gas [reaction (R6)]. During the second stage, the Co3O4 generated was consumed by the formation of Li2Co(SO4)2 and CoO with the overall reaction (R7). As there are no thermodynamic data for Li2Co(SO4)2, reactions (R8) to (R12) were then used as references to describe the process. As Fig. 7b shows, Co3O4 was reduced to produce CoO and CoSO4 by either reaction (R8) or (R9), and the CoSO4 generated was combined with Li2SO4 to produce Li2Co(SO4)2 by reaction (R10). The sub-reactions (R8), (R9), and (R10) were only used to better understand the roasting process. As no CoSO4 was detected during the roasting reactions, Li2Co(SO4)2 was believed to be formed directly by reaction (R7). The CoO generated may also have been sulfated by reactions (R11) and (R12) to produce CoSO4 and to accelerate the production of Li2Co(SO4)2. Finally, the sulfation roasting reactions would be completed in stage 3 to obtain the end products of Li2SO4, Li2Co(SO4)2, and CoO. This is the reason for the conversion calculations in Fig. 3c. Based on the overall reaction (R1), the conversion ratio was recalculated for a roasting time of 30 min to 240 min, and the results are plotted together in Fig. 3c. The conversion ratio rapidly reached 90% for 30 min and then gradually increased close to 100% with a roasting time further increased beyond 30 min.
Fig. 7

Relationship between ∆Gθ (kJ mol−1) and temperature (T, °C) for different reactions (R2) to (R12). (a) Reactions taking place during stage 1: Gibbs energy of reaction versus temperature;41 (b) reactions taking place during stage 2: Gibbs energy of the reaction versus temperature41

Stage 1Gθ in kJ mol−1, temperature T in °C)
$$ 4{\text{LiCoO}}_{2} \left( {\text{s}} \right)\, = \,2{\text{Li}}_{2} {\text{O }}\left( {\text{s}} \right)\, + \,4{\text{CoO }}\left( {\text{s}} \right)\, + \,{\text{O}}_{2} \left( {\text{g}} \right)\quad \quad \Delta G^{\theta } \, = \,489.00476 - 0.30411T[41]\quad \left( {R2} \right) $$
$$ 12{\text{LiCoO}}_{2} \left( {\text{s}} \right)\, = \,6{\text{Li}}_{2} {\text{O }}\left( {\text{s}} \right)\, + \,4{\text{Co}}_{3} {\text{O}}_{4} \left( {\text{s}} \right)\, + \,{\text{O}}_{2} \left( {\text{g}} \right)\quad \quad \Delta G^{\theta } \, = \,811.59349 - 0.23849T[41]\quad \left( {R3} \right) $$
$$ 2{\text{SO}}_{2} \left( {\text{g}} \right)\, + \,{\text{O}}_{2} \left( {\text{g}} \right)\, = \,2{\text{SO}}_{3} \left( {\text{g}} \right)\quad \quad \Delta G^{\theta } \, = \, - 146.2697\, + \,0.18775T[41]\quad \left( {R4} \right) $$
$$ \text{6LiCoO}_{\text{2}} \left( \text{s} \right)\,\text{ + }\,\text{3SO}_{\text{2}} \left( \text{g} \right)\,\text{ + }\,\text{O}_{\text{2}} \left( \text{g} \right)\,\text{ = }\,\text{3Li}_{\text{2}} \text{SO}_{\text{4}} \left( \text{s} \right)\,\text{ + }\,\text{2Co}_{\text{3}} \text{O}_{\text{4}} \left( \text{s} \right)\quad \quad \Delta G^{\theta } \, = \, - 974.36564\, + \,0.60604T[41]\quad \left( {R5} \right) $$
$$ \text{12LiCoO}_{\text{2}} \left( \text{s} \right)\,\text{ + }\,\text{6SO}_{\text{3}} \left( \text{g} \right)\,\text{ = }\,\text{6Li}_{\text{2}} \text{SO}_{\text{4}} \left( \text{s} \right)\,\text{ + }\,\text{4Co}_{\text{3}} \text{O}_{\text{4}} \left( \text{s} \right)\,\text{ + }\,\text{O}_{\text{2}} \left( \text{g} \right)\quad \quad \Delta G^{\theta } \, = \, - 1509.92219\, + \,0.64882T[41] \, \quad \left( {R6} \right) $$
Stage 2
$$ \text{3Co}_{\text{3}} \text{O}_{\text{4}} \left( \text{s} \right)\,\text{ + }\,\text{7SO}_{\text{2}} \left( \text{g} \right)\,\text{ + }\,\text{2O}_{\text{2}} \left( \text{g} \right)\,\text{ + }\,\text{7Li}_{\text{2}} \text{SO}_{\text{4}} \left( \text{s} \right)\,\text{ = }\,\text{7Li}_{\text{2}} \text{Co}\left( {\text{SO}_{\text{4}} } \right)_{\text{2}} \left( \text{s} \right)\,\text{ + }\,\text{CoO }\left( \text{s} \right)\quad \left( {R7} \right) $$
$$ 3{\text{Co}}_{ 3} {\text{O}}_{4} \left( {\text{s}} \right)\, + \,7{\text{SO}}_{2} \left( {\text{g}} \right)\, + \,2{\text{O}}_{2} \left( {\text{g}} \right)\, = \,7{\text{CoSO}}_{4} \left( {\text{s}} \right)\, + \,{\text{CoO }}\left( {\text{s}} \right)\quad \quad \Delta G^{\theta } \, = \, - 1417.82422\, + \,1.4114T[41]\quad \, \left( {R8} \right) $$
$$ 3{\text{Co}}_{3} {\text{O}}_{4} \left( {\text{s}} \right)\, + \,{\text{SO}}_{2} \left( {\text{g}} \right)\, = \,{\text{CoSO}}_{4} \left( {\text{s}} \right)\, + \,2{\text{CoO }}\left( {\text{s}} \right)\quad \quad \Delta G^{\theta } \, = \, - 108.91481\, + \,0.10537T[41] \, \quad \left( {R9} \right) $$
$$ {\text{Li}}_{2} {\text{SO}}_{4} \left( {\text{s}} \right)\, + \,{\text{CoSO}}_{4} \left( {\text{s}} \right)\, = \,{\text{Li}}_{2} {\text{Co}}\left( {{\text{SO}}_{4} } \right)_{2} \left( {\text{s}} \right)\quad \left( {R10} \right) $$
$$ 2{\text{CoO }}\left( {\text{s}} \right)\, + \,2{\text{SO}}_{2} \left( {\text{g}} \right)\, + \,{\text{O}}_{2} \left( {\text{g}} \right)\, = \,2{\text{CoSO}}_{4} \left( {\text{s}} \right)\quad \quad \Delta G^{\theta } \, = \, - 545.53989\, + \,0.54765T[41] \, \quad \left( {R11} \right) $$
$$ {\text{CoO }}\left( {\text{s}} \right)\, + \,{\text{SO}}_{3} \left( {\text{g}} \right)\, = \,{\text{CoSO}}_{4} \left( {\text{s}} \right)\quad \quad \Delta G^{\theta } \, = \, - 199.6351\, + \,0.17995T[41] \, \quad \left( {R12} \right) $$

Conclusion

Sulfation roasting followed by water leaching has been proposed for the recycling of spent LIBs. The reaction mechanism was studied by the roasting of synthetic LiCoO2 powder in 10% SO2-1% O2-89% Ar gas atmosphere at 700°C. The reaction patterns and corresponding microstructures were analyzed by XRD and SEM–EDS, while the Li and Co contents in the pregnant solution were characterized by AAS analysis. Based on the experimental results, the reaction mechanism under the present experimental condition was concluded as follows: LiCoO2 powder was first converted to Li2SO4 and Co3O4; the produced Co3O4 was further reduced as CoO or combined with Li2SO4 to form Li2Co(SO4)2. In the end, the products of Li2SO4, Li2Co(SO4)2, and CoO were obtained. The experimental results were quite different from the thermodynamic predictions where Li2SO4 and CoSO4 were calculated as the final products, as Li2Co(SO4)2 was not presented in the database. The achieved results suggest that sulfation roasting can provide a method for direct leaching of Li for improved Li recovery from battery waste. However, only 17.4% of Co could be extracted into the water, indicating a need for consequent development of an acid leaching process. The results from the present work are not only important for recycling of spent LIBs, but also can serve as a basis for the thermodynamic modeling of an Li-Co-O-S system. Moreover, the experimental results can also provide a method for consuming the SO2 gas generated from metallurgical smelting processes, e.g., the copper matte converting process.

Notes

Acknowledgements

Open access funding provided by Aalto University. This work was financed by the Aalto University School of Chemical Engineering and utilized the Academy of Finland’s RawMatTERS Finland Infrastructure (RAMI), based jointly at Aalto University, GTK Espoo, and VTT Espoo.

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Authors and Affiliations

  1. 1.Department of Chemical and Metallurgical Engineering, School of Chemical EngineeringAalto UniversityEspooFinland

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