3.1.1. Thermodynamic Analysis of Oxidation Acid Leaching Process
To illustrate the feasibility of the oxidation acid leaching system, a thermodynamic analysis of the process was performed. The electrode potential indicates the oxidizing capacity of the oxidizing agent and the reducing capacity of the reducing substance, which determines whether the redox reaction can proceed and the order in which the reaction proceeds. The following are the half-reactions of the ions involved in the oxidation-acid leaching process and their electrode potentials in the standard state.
The electrode potential difference ΔE between the oxidizing agent and the reducing agent reflects the driving force of the chemical reaction. If the electrode potential difference ΔE is larger, it indicates that the reaction driving force is larger. The standard electrode potential difference ΔE
θ for the oxidation of Ni
2+, Co
2+, [Co(NH
3)
6]
2+, Mn
2+, Ni(OH)
2 by S
2O
82− in the oxidation acid leaching system and all possible reaction equations are shown below:
The order of the above standard electrode potential difference is ΔE4θ > ΔE6θ > ΔE7θ > ΔE5θ > ΔE2θ > ΔE1θ > ΔE3θ. The smallest ΔE3θ represents the oxidation of Co2+ to Co3+ by S2O82−. But due to the presence of NH4+, the oxidation of Co2+ to Co3+ is transformed into the oxidation of [Co(NH3)6]2+ to [Co(NH3)6]3+, the standard electrode potential difference of the process is 1.902 V, and the reaction driving force is maximum. ΔE2θ and ΔE1θ are the smallest, all of which are the Ni2+ being oxidized, indicating that the driving force for the oxidation process of Ni2+ is minimal. Therefore, in the subsequent oxidation acid leaching experiment, some Ni2+ was found to be leached into the solution, which is also consistent with the theory. The above theoretical analysis proves that S2O82− can not only maintain the oxidation leaching environment as strongly oxidizing agent, but also oxidize the low-valent ions such as Ni2+, Co2+, [Co(NH3)6]2+, and Mn2+ dissolved in the leaching solution to high-valent insoluble substances, so as to realize the selective and efficient leaching of lithium from spent ternary positive electrode materials.
In the oxidation acid leaching slurry with alkali precipitation of Ni2+, the NaOH addition product should be Ni(OH)2, while the XRD Figure 5a shows that the reaction product is NiO2. From Equations (1) and (9), NiO2 is generated by the oxidation of Ni(OH)2 by S2O82−, and the standard potential difference of this process is ΔEθ = 1.52 V, which has a large reaction driving force.
3.1.2. Dynamics Analysis of Oxidation Acid Leaching Process
In order to gain an in-depth understanding of the whole oxidation acid leaching process, the study of the kinetics of the leaching of valuable metals is essential. The leaching of valuable metals is the process of moving metal ions from a solid metal oxide into the liquid phase. The leaching reaction process proceeds from the outer surface of the particle toward the inner core, and the particle slowly shrinks until the reaction is completed. This process is a combination of mass transfer, diffusion, and chemical reaction. Originally used to analyze the kinetics of crystallization processes and later applied to describe the kinetics of leaching reactions for various minerals, the Avrami equation model will be introduced in this section to describe the leaching kinetics of positive electrode materials for decommissioned lithium-ion batteries. We understand the reaction mechanism of the whole oxidation acid leaching process from the leaching kinetics. The role of the oxidizing agent in this leaching system is to inhibit the leaching of manganese and cobalt, and their leaching efficiencies are too low to study their leaching kinetics. Some nickel elements in the spent ternary material will enter the leaching solution, but the process involves redox reactions in addition to acid leaching, and its leaching kinetics cannot be studied singularly. Therefore, we only study the leaching kinetics of lithium in spent ternary materials. The reaction rate control steps are usually surface chemical reaction control (Equation (24)), diffusion control (Equation (25)), logarithmic rate control (Equation (26)), and the Avrami equation (Equation (27)).
where
x is the fraction of the reaction,
k1 to
k4 are the reaction rate constants (h
−1),
t is the leaching time (h), and
n is determined by the fitting results.
The apparent activation energy (E
a) of the valent metal represents the difficulty of the reaction and can be determined from the Arrhenius equation as follows:
where
k is the reaction rate constant (h
−1), E
a is the surface activation energy (kJ mol
−1), and
T is the absolute temperature (K).
It can be seen from the above equation (Equation (28)) that lnk and 1/T are linearly related, and the apparent activation energy of metal leaching can be found by plotting lnk and 1/T with a slope of −Ea/R.
The kinetics of lithium leaching from spent ternary materials were studied with different reaction times (0–9 h) and temperatures (20–65 °C). Other conditions were controlled at the optimum level, and the leaching data were substituted into the four models (Equations (20)–(23)) with
t or ln
t as the horizontal coordinates and (−ln(1 −
x))
2, 1 − (2/3)
x−(1 −
x)
2/3, (1 −
x)
1/3, ln(−ln(1 −
x)) as the vertical coordinates for the graphs, respectively, to obtain the kinetic equations of lithium leaching. The results are shown in
Figure 1. The specific parameters of the fitting are in
Table 1, where the value of R
2 reflects the degree of fitting.
It can be seen from
Figure 1a–c and
Table 1 that the chemical reaction control model and the internal diffusion control model have poor correlation fits, while the Avrami equation model (R
2 > 0.98) has a better fit correlation compared to the other models. The Avrami equation model has the best fitting correlation, indicating that the kinetics is mainly controlled by the inverse process of the crystal. This also demonstrates that the Avrami equation can be used to explain the leaching of solids containing multiple metallic elements in the liquid phase system. The fits of the other models are good at low temperatures, but decrease as the temperature increases. The intercept of the Avrami equation is ln
k, and from the fitting results,
Table 1 shows that the intercept increases sequentially from a low to a high temperature, indicating that the reaction rate constant increases with increasing temperature. This also indicates that increasing the reaction temperature is beneficial to leaching.
A plot of ln
k versus 1/
T was obtained by fitting the temperature and rate constants from the Avrami equation model, as shown in
Figure 2. The slope of the straight line is −E
a/R. R
2 = 0.98 indicates that the fit is very good. The apparent activation energy of Li leaching in the leaching system can be calculated to be 46 kJ/mol, indicating that the reaction rate in the leaching process is controlled by the surface chemistry.
3.1.3. Optimization of Oxidation Acid Leaching Reaction Conditions
The concentrations of the oxidizer and acid, as well as the reaction time, temperature, and solid–liquid ratio, all have effects on the leaching efficiency of valuable metal ions. In order to understand the whole process, it is necessary to conduct single-factor experiments on the leaching process, and the results are shown in
Figure 3.
The effects of sulfuric acid concentration on the leaching efficiency of metals such as lithium, nickel, cobalt, and manganese were studied. The role of acid in this leaching system is to destroy the structure of the waste material and to leach the lithium from the material into the leaching solution. The leaching of other elements cannot be avoided in this process. It can be seen from
Figure 3a that the leaching efficiencies of Li, Ni, and Co all increased with increasing acid concentration, and the change in Mn leaching efficiency was not obvious. When the sulfuric acid concentration was 1 mol L
−1, the leaching efficiency effect of lithium was excellent, reaching 99.6%, but the leaching efficiency of nickel and cobalt also reached about 50%, and the effect of lithium selective extraction could not be achieved. When the acid concentration was 0.1 mol L
−1, the lithium leaching efficiency reached 97.2%; the manganese leaching efficiency was extremely low; the cobalt leaching efficiency was below 10%; and the nickel leaching efficiency was at a relatively low level, 28%. The leaching efficiencies of cobalt and nickel increased when the concentration of acid increased, while the leaching efficiency of lithium decreased when the concentration of acid decreased. Therefore, a 0.1 mol L
−1 acid concentration was chosen as the optimum acid concentration.
The effects of different oxidant concentrations on the leaching efficiency of lithium, nickel, cobalt and manganese metals was investigated. The role of the oxidant in this leaching system was to inhibit the leaching of transition metal elements. Sulfuric acid leaching is not selective, and the addition of the oxidant reduces the leaching of transition metal elements so that the lithium in the spent ternary materials can be leached selectively. Firstly, only 0.1 mol L
−1 sulfuric acid was used to leach the spent ternary materials, and it was found that the leaching under this condition was not selective. The leaching efficiency of lithium was less than 50%, and the leaching efficiencies of nickel, cobalt, and manganese also reached more than 20%. As the concentration of oxidant increased, the leaching efficiency of lithium increased rapidly, the leaching efficiency of nickel increased slowly, and the leaching efficiencies of cobalt and manganese decreased. This indicates that the high concentration of ammonium persulfate can inhibit the leaching of cobalt and manganese and slow down the leaching of nickel, but not at a lower level. There was a slight increase after the decrease of cobalt leaching efficiency, as shown in
Figure 3b, which we believe was due to an error during the experiment because the temperature could not be kept the same for each group of experiments. When the oxidant concentration was 0.2 mol L
−1, 98.7% of the lithium in the spent ternary material could be leached into the leaching solution, and the leaching efficiencies of cobalt, nickel, and manganese were maintained at a low level. When the oxidant concentration was less than 0.2 mol L
−1, the lithium leaching efficiency could not reach the requirement, and the cobalt leaching efficiency was also relatively high. When the oxidant concentration was greater than 0.2 mol L
−1, the leaching of lithium, nickel, cobalt, and manganese did not change much. Thus, the optimal oxidant concentration was chosen to be 0.2 mol L
−1.
The effects of different reaction times on the leaching efficiencies of metals such as lithium, nickel, cobalt, and manganese were investigated. Since the leaching system used a low concentration of acid, which has a limited ability to damage the structure of the material, longer reaction times were required. The reaction times were controlled at 2–12 h. It can be seen from
Figure 3c that the length of the reaction time had little effect on the leaching of nickel, cobalt and manganese elements, while the leaching efficiency of lithium became higher as the reaction time increased. The lithium leaching efficiencies were 96.6% at the reaction time of 5 h, 98.0% at the reaction time of 6 h, and 98.2% at the reaction time of 7 h. The lithium leaching efficiency was low when the reaction times were 5 h and below, and when the reaction times were 7 h and above, the lithium leaching efficiency was maintained at a high level with little variation, so 6 h was chosen as the optimal reaction time to ensure high lithium leaching efficiency and high selectivity, as well as to relatively reduce the heating energy and time costs.
The effects of different reaction temperatures on the leaching efficiencies of lithium, nickel, cobalt, and manganese metals were investigated. The reaction temperature was controlled at 25–95 °C, and graphs of the variation in the leaching efficiency of lithium, nickel, cobalt, and manganese at different reaction temperatures were obtained (
Figure 3d). As shown in
Figure 3d, the lithium leaching efficiency was low at a low temperature, and there was no selectivity. The leaching efficiency of lithium increased rapidly with the increase in temperature. This may have been due to the enhanced mass transfer effect of increasing temperature, which led to faster leaching of lithium. When the temperature was 60–70 °C, the leaching efficiencies of cobalt and manganese decreased rapidly. This indicates that the oxidation leaching system had no or a weak inhibitory effect on the leaching of transition metal elements at a low temperature, and the inhibitory effect increased with the increase in temperature. When the temperature increased to a certain degree, the leaching efficiency of transition metal elements could be limited to a low level (less than 10%), and the leaching of lithium had a certain selectivity. When the temperature was lower than 65 °C, the lithium leaching efficiency was lower than 92%, the cobalt and manganese leaching efficiencies were larger, and the lithium selectivity was smaller. When the temperature was 65 °C, the lithium leaching efficiency reached 98.7%, while the cobalt and manganese leaching efficiencies were lower than 5%, and the lithium leaching selectivity was higher. When the temperature was higher than 65 °C, the lithium and cobalt and manganese leaching efficiencies did not change much, but the nickel leaching efficiency continued to grow. Therefore, the optimum reaction temperature of 65 °C was determined to ensure high lithium leaching efficiency and high selectivity, and also to relatively reduce heating energy consumption.
The effect of different solid–liquid ratios on the leaching efficiencies of lithium, nickel, cobalt, and manganese metals was investigated. A larger solid–liquid ratio allowed for a higher concentration of lithium solution in the leachate, reducing the cost of the concentration process and facilitating the preparation of lithium carbonate at a later stage. However, it can be seen from
Figure 3e that the lithium leaching decreased when the solid–liquid ratio increases. Therefore, a suitable solid–liquid ratio was necessary to achieve both high lithium leaching efficiency and high selectivity. As shown in
Figure 3e, the leaching efficiencies of lithium, nickel, cobalt, and manganese were 98.2, 25.3, 2.7, and 0.03%, respectively, when the solid–liquid ratio was 25 g L
−1. When the solid–liquid ratio was less than 25 g L
−1, the lithium leaching efficiency and selectivity were also at a high level, but the low solid–liquid ratio meant that the concentration of lithium ions in the leachate was low, increasing the evaporation concentration cost. When the solid–liquid ratio was greater than 25 g L
−1, the lithium leaching efficiency decreased rapidly. Therefore, the solid–liquid ratio of 25 g L
−1 charging was chosen as the best solid–liquid ratio for the reaction, ensuring a high Li
+ concentration in the leachate, but also a high lithium leaching efficiency and good selectivity.
It can be concluded from the above series of experiments that the optimal reaction conditions for this reaction are
c[H
2SO
4] = 0.1 mol L
−1,
c[(NH
4)
2S
2O
8] = 0.2 mol L
−1,
t = 6 h,
T = 65 °C, and a dosing solid–liquid ratio of 25 g L
−1. The experimental leaching efficiencies of Li, Ni, Co, and Mn under these conditions were 98.7, 30.0, 3.5, and 0.1%, as shown in
Figure 3f. The lithium leaching efficiency was at a high level, while the leaching efficiencies of both cobalt and manganese were low, indicating that the lithium leaching selectivity was good. Then, by adding sodium hydroxide to the leaching solution to precipitate Ni
2+, a pure lithium solution was obtained for the preparation of Li
2CO
3.
3.1.4. Physical Phase Analysis of Oxidation Acid Leaching Process
The SEM images of the raw spent ternary positive electrode material, the direct filtration slag after oxidation acid leaching, and the precipitation slag after oxidation acid leaching with sodium hydroxide are shown in
Figure 4. It can be seen from
Figure 4a–c that the particles of the spent ternary positive electrode material were broken, irregular in shape, and agglomerated. It can be observed in
Figure 4d–f that, after oxidation acid leaching, the surface of the particles became smooth, and the agglomerated large particles were dispersed and had a certain sphericity. The oxidation acid leaching treatment was followed by adding sodium hydroxide to the beaker to adjust the pH of the solution so that the nickel ions and OH
− in the solution combined to form the precipitate. The resulting mixed slag contained nickel hydroxide and the ternary materials of delithiation, and their SEM images are shown in
Figure 4g–i. Due to the treatment of strong alkali, the surface of the material was not so smooth, and the particle shape was irregular. The leached nickel ions were precipitated by adding sodium hydroxide to the leaching slurry to adjust the pH, and a solid slag was obtained after the reaction was completed, which was used as a precursor for the ternary material. The precursor and lithium source (lithium hydroxide monohydrate) were mixed thoroughly with a ball mill and calcined under an oxygen atmosphere to prepare the regenerated ternary positive electrode material (R-NCM523). The SEM images of the regenerated material are shown in
Figure 4a–c, and they show a smoother particle surface, relatively more uniform particle size, and better sphericity compared to the oxidized leach slag.
The XRD patterns before and after the oxidation acid leaching are shown in
Figure 5. Specifically, the black curve is the XRD pattern of the spent ternary positive electrode material (NCM523), the red curve is the XRD pattern of the solid slag obtained by direct filtration after the oxidation acid leaching, and the blue curve shows the XRD pattern of the leached slag obtained by adding NaOH to adjust the pH to 11 after the oxidation acid leaching. It can be observed that the XRD peak patterns and positions of the oxidation leaching slag and the spent ternary material are similar, indicating that the structure of the slag obtained from the oxidation acid leaching of NCM523 material did not change drastically, and only the lithium in the lamellar structure of the material was stripped out, maintaining the lamellar structure of NCM523, as shown in
Figure 5b. The blue curve in
Figure 5a shows only two peaks in the dashed box, more than the red curve. These two peaks represent the NiO
2 generated by the oxidation of Ni
2+ through oxidation acid leaching during the process of alkali precipitation, and the PDF card below can be a good match. It is known from the thermodynamic analysis section that the standard electrode potential for Ni(OH)
2 to be oxidized to NiO
2 is 0.49 V, while the oxidation potential of S
2O
82− is 2.01 V. The excess oxidant from the oxidation acid leaching process was sufficient to oxidize Ni(OH)
2 to NiO
2, and the theory is consistent with reality.
In addition, ICP-OES was used to test the Ni, Co, and Mn contents in the slag after oxidation acid leaching followed by NaOH precipitation, and Ni:Co:Mn = 5:2:3 (molar ratio) was obtained, which is consistent with our experimental concept and can be used for the preparation of regenerated positive electrode material (R-NCM523).
3.1.5. Analysis of the Mechanism of Oxidation Acid Leaching
The XPS spectra comparing the surface of the scrap NCM523 raw material and the oxidation acid leaching slag without alkali sink are shown in
Figure 6. The XPS pattern of Ni 2p is shown in
Figure 6a. The binding energy of the spent NCM523 material had two main peaks of Ni 2p
3/2 and Ni 2p
1/2 at 854.0 eV and 872.0 eV, and two satellite peaks with binding energies of 860.9 eV and 879.0 eV, which are close to the binding energy data of Ni
2+ [
32,
33]. The two strong peaks at binding energies of 855.5 eV and 873.1 eV prove the presence of Ni
3+. The peaks of Ni
2+ disappeared from the XPS spectrum of the powder after the oxidation acid leaching treatment, and only the peaks of Ni
3+ remained, indicating that after oxidation acid leaching treatment, some Ni
2+ leached into the solution and some Ni
2+ was oxidized to Ni
3+.
The XPS pattern of Co 2p is shown in
Figure 6b. There are two main peaks of Co 2p
3/2 and Co 2p
1/2 at 780.3 eV and 795.3 eV [
34] in the XPS pattern of the spent NCM523 material at the binding energy, and two weaker peaks at 789.3 eV and 804.3 eV at the binding energy belong to Co
3+. The two peaks with binding energies of 782.5 eV and 797 eV belong to Co
4+. The XPS patterns of Co 2p before and after oxidation acid leaching did not change significantly, indicating that the cobalt remained unchanged in the original structure both before and after leaching, which is also consistent with the minimal amount of cobalt in the leachate. The XPS pattern of Mn 2p is shown in
Figure 6c. The binding energy of the spent NCM523 material has two main peaks of Mn 2p
3/2 and Mn 2p
1/2 at 642.5 eV and 653.8 eV, which are close to the binding energy data of Mn
4+ [
32,
35]. The XPS patterns of Mn 2p did not change significantly from before to after oxidation leaching, indicating that Mn remained unchanged in the original structure both before and after leaching, which is also consistent with the minimal Mn content in the leachate. The XPS patterns before and after the oxidative leaching of the scrap NCM523 can show that the Ni
2+ in the scrap positive electrode material was partially leached into the solution and partially oxidized to high valence. While both cobalt and manganese were originally maintained at high valence, the leaching retained them in the original structure, and lithium leached into the solution to achieve selective lithium extraction.