Introduction

The extensive use of fossil fuels has led to increasingly serious environmental pollution problems. The pursuit of a green, safe, economically sustainable, and clean energy source has become a shared goal among all countries worldwide [1, 2]. In recent years, lithium-ion batteries have been widely used and promoted as a power source for new energy transportation and electronic equipment. However, significant environmental pollution problems and safety hazards exist in both their production and actual application [3, 4]. Aqueous zinc-ion batteries (AZIBs) based on a mild aqueous solution as an electrolyte have been favored by researchers due to their environmental friendliness, low cost, resourcefulness, high theoretical specific capacity, and lower potentials [5,6,7,8,9]. There are three main types of cathode materials for AZIBs [10]: manganese-based oxides [11, 12], vanadium-based oxides [13,14,15,16,17], and Prussian blue analogs [18, 19]. Among them, manganese-based oxides are the most common cathode materials for AZIBs, and MnO2 is recognized as the primary cathode material for AZIBs. In order to enhance battery performance, various methods such as doping and mixing have been utilized to improve the structure of cathode materials [20,21,22,23]. Notably, the electrolyte is also a key component of batteries, providing a conducive working environment to ensure high compatibility and reversible cycling of the battery components. However, factors hindering the detachment of Zn2+, such as cathodic dissolution, uncontrollable by-products, uncertainty in the storage mechanism, and insufficient energy density, still need to be resolved. These factors considerably limit the reversible specific capacity and cycling life of AZIBs [24,25,26,27].

Enhancing the performance of AZIBs on the basis of manganese-based cathode materials based on electrolyte modulation strategies has been extensively studied by scholars [28,29,30,31,32]. The first is to compare the effect of electrolytes with different anion compositions on the performance of batteries. Hu’s [33] study found that the anion CF3SO3 in Zn(CF3SO3)2 is bulky, which reduces solvation, and that CF3SO3 has less interaction with water compared to the ZnSO4 electrolyte, which enhances electrochemical performance. Using zinc gluconate as an electrolyte, Xu [34] found that it not only stabilizes the supply of Zn2+, but also acts as an interfacial stabilizer to provide gluconate anions, creating an artificially stabilized anionic interface and forming dendrite-free deposits; secondly, the addition of metal cation additives can effectively alleviate the dissolution of cathode materials according to the dissolution balance mechanism. Deng’s [35] study achieved high specific capacity (326 mAh·g−1 at 100 mA·g−1) and excellent long-term cycling performance (stable capacity after 700 cycles at 2000 mA·g−1) based on the prepared MnO2@CC cathode with electrolyte modulation with 3 M ZnSO4 + 0.1 M MnSO4. Zhang [36] innovatively used Mn2+ and Li+ bimetallic anode electrolyte modulation to achieve a battery capacity of more than 300 mAh·g−1 with 1 M ZnSO4 + 1 M LiSO4 + 0.1 M MnSO4 as the electrolyte under the synergistic effect of Mn2+ and Li+ and up to 2000 long-term stability cycles at a high current density of 2 A·g−1. In addition, organic electrolyte additives (monosodium glutamate, threonine, eco-friendly silk peptides, etc.) play an important role in regulating the internal structure of solvents and inhibiting zinc dendrites in batteries [37,38,39,40,41,42]. It can be seen that in order to obtain long-life and highly stable AZIBs, attention must be paid to the electrolyte improvement strategy, and manganese-based oxides or hybrid cathode materials formed by them and carbon substances have excellent electrochemical performance under suitable electrolytes.

However, the theoretical specific capacity of conventional one-electron reactions based on the Mn4+/Mn3+ redox couple is usually about 308 mAh·g−1, whereas it can be increased to 616 mAh·g−1 by a two-electron conversion mechanism (Mn4+/Mn2+). In order to construct a direct two-electron conversion mechanism of Mn4+/Mn2+ and enhance the theoretical discharge-specific capacity of AZIBs, some scholars have made their own efforts, and through their respective innovative experiments, they have successfully realized the direct conversion of MnO2 to Mn2+ at high operating voltage, which improves the discharge-specific capacity and the cycling life of AZIBs. Therefore, it is theorized that increasing the work potential of AZIBs by experimental methods will enhance the Mn4+/Mn2+ two-electron conversion reaction [43, 44]. Unlike them, some scholars constructed the Mn4+/Mn2+ two-electron conversion mechanism not by realizing a high operating voltage but by improving the structural properties of the cathode material or by electrolyte modulation. Li’s study developed a nanoflower-like MnO2/C composite as the anode material with 2.0 M ZnSO4 + 0.5 M MnSO4 as the electrolyte, and the results showed that the zinc-ion batteries with MnO2/C as the cathode material could carry out a deep and fast reaction through the Mn4+/Mn2+ two-electronic pathway, which was largely attributed to the advantages of the anode material such as fewer agglomerations, a larger specific surface area, and the presence of water of crystallization [45]. Zeng used an electrolyte modulation strategy and chose a mixed electrolyte salt of Zn(CH3COO)2 and Mn(CH3COO)2 for the two-electron redox reaction of Mn4+/Mn2+ [46]. Zhong’s study used acetate ions for electrolyte modulation, and they added CH3COONa to the electrolytes of ZnSO4 and MnSO4 to achieve the MnO2/Mn2+ conversion, the reason for this is reflected in the role of acetate ions, which promote the deposition of Mn2+ [47].

In this paper, we fabricated a hybrid of β-MnO2/3D graphene-carbon nanotube cross-link (abbreviation: β-MnO2/3D GPE-CNT) cathode material using a simple mechanical ball-milling method. This material exhibited excellent performance. Additionally, we introduced MnSO4 and H2SO4 additives to the ZnSO4 electrolyte. This method promotes the formation of a Mn4+/Mn2+ two-electron conversion mechanism while ensuring the structural stability of cathode materials. In addition, we investigated the effects of different concentrations of H2SO4 on the electrochemical performance of the batteries. The results showed that the stabilized operating potential and discharge performance of the batteries improved with the addition of H2SO4. Specifically, batteries with 0.1 M H2SO4 in the electrolyte exhibited a reversible discharge-specific capacity of up to 536.07 mAh·g−1 at a current density of 100 mA·g−1. Furthermore, the activated batteries demonstrated a reversible specific capacity of 85.11 mAh·g−1 even under a high current density of 1 A·g−1, with a capacity retention rate of 88.3% after 1000 cycles. This work aims to offer a solution for large-scale energy storage applications using high-performance rechargeable aqueous Zn/MnO2 batteries.

Experimental materials and methods

The original specimens used for the experiment were as follows: manganese dioxide (MnO2, Xilong Science, China); zinc sulfate (ZnSO4), manganese sulfate (MnSO4), and N-methyl-2-pyrrolidone (NMP) were purchased from Aladdin, Italy; polyvinylidene fluoride (PVDF, Arkema, France); 3D graphene-carbon nanotubes (for microstructure see [48]); conductive carbon black (Super P, DENKA, Japan); parts of CR2032 button batteries.

The detailed preparation process of β-MnO2/3D GEP-CNT hybrid cathode materials obtained by ball milling is described in [48, 49]. The mass ratio of β-MnO2 to 3D GPE-CNT was 9:1, and the actual ball milling time was 2.5 h. The ball-milled cathode material, Super P, and PVDF were mixed homogeneously according to the mass ratio of 7:2:1 and then dripped into the appropriate amount of NMP solution, which was fully ground in an onyx mortar to obtain the slurry of cathode wafers. The slurry was uniformly coated on the surface of 316 stainless steel foil, and then placed in a vacuum drying oven at 110 °C for 12 h. A cutting machine was used to cut the dried specimen sheet into a circular sheet with a diameter of about 14 mm as the positive electrode sheet, and the average mass density of the active substance on the positive electrode sheet was about 0.49 mg·cm−2. Then, it is assembled with zinc sheet negative electrode, electrolyte, and glass fiber diaphragm to form CR2032 type button batteries, where the electrolyte is (2M ZnSO4 + 0.5M MnSO4 + 0.05, 0.1, 0.2, 0.3 M H2SO4) solution respectively.

X-ray diffraction analysis (XRD, SmartLab), field emission scanning electron microscope (FSEM, Hitachi S-4800), transmission electron microscope (TEM, JEOL JEM 2800), laser particle size analyzer (Malvern 3000), and specific surface pore size analyzer (JW-BK200B) were used to test the phase structure, particle morphology, atomic arrangement, particle size distribution, and specific surface area size of the β-MnO2/3D GEP-CNT hybrid anode material, respectively. The assembled batteries were allowed to stand for more than 6 h. Constant-current charge/discharge tests were performed in a Neware battery tester (Model CT-4008) at different current densities in the range of 100 mA·g−1 to 1A·g−1, and electrochemical impedance spectroscopy was carried out in an electrochemical workstation (Model CHI660) with frequency scans ranging from 0.01 Hz to 100 kHz. The cyclic voltammetry (CV) curves were tested at scanning rates of 0.1, 0.2, 0.3, 0.4, and 0.5 mv·s−1.

Results and discussion

The results of the microstructure tests are described in detail in and will not be repeated here [48, 49]. As shown in Fig. 1a–c, the results of SEM and TEM tests showed that the hybrids after ball milling were distributed as spherical particles, the phenomenon of agglomeration was obviously reduced, and the ball milling greatly reduced the particle size of the anode material, which led to the increase of the specific surface area of the material. As shown in Fig. 1d, the XRD patterns related to MnO2 in the β-MnO2/3D GEP-CNT hybrids matched the standard card (JCPDS: 39-0375) for β-MnO2, and the phase structure of the samples was not significantly altered before and after ball milling. The results of the particle size test are given in Fig. 1e, and the average particle size of the sample obtained by the laser particle size analyzer was 20.33 μm. XPS tests of the ball-milled styles are given in Fig. 1f, and the results show that the peak positions and the peak value of Mn2p did not change significantly after ball milling.

Fig. 1
figure 1

Microcosmic characterization Chart. a SEM image of β-MnO2/3D GEP-CNT; b and c TEM image of β-MnO2/3D GEP-CNT; d XRD image of β-MnO2/3D GEP-CNT; e particle size test image of β-MnO2/3D GEP-CNT; f XPS image of β-MnO2/3D GEP-CNT

Inspired by the above, the deepening of the MnO2/Mn2+ conversion reaction can also be effectively promoted under the suitable cathode material or electrolyte, thus providing higher reversible specific capacity and stable charging/discharging cycles for AZIBs. In our previous studies, we have demonstrated that β-MnO2/3D GEP-CNT cathode materials have properties such as low agglomeration and high specific surface area, which are favorable for Zn2+ insertion and extraction, and the reversible specific capacity of the batteries is improved compared with that of ordinary β-MnO2 cathode materials [48]. With 2.0 M ZnSO4 + 0.5 M MnSO4 as the electrolyte, the specific capacity of the batteries reached 521.91 mAh·g−1 after activation, and we proved the existence of an indirect conversion mechanism of MnO2/Mn2+ by electrochemical tests [49]. In order to further deepen this two-electron conversion mechanism, we continued to add different concentrations of H2SO4 to the above electrolyte. The capacity decay curves of the batteries at a current density of 100 mA·g−1 with different concentrations of H2SO4 solutions pre-added to the electrolyte are shown in Fig. 2a. The discharge-specific capacity of the β-MnO2/3D GEP-CNT cathode material reached 302.37 mAh·g−1 after activation when 2.0 M ZnSO4 + 0.5 M MnSO4 + 0.05 M H2SO4 solution was used as the electrolyte, which was higher than that when ZnSO4 solution was used as the electrolyte alone, and the capacity decay was very slow when the batteries were stabilized. The combination of previous studies suggests that it is the MnSO4 in the electrolyte that plays a role, and that it inhibits the capacity degradation of the batteries well. However, the addition of 0.05 M H2SO4 did not further enhance the performance of the batteries, such as the activation rate and reversible specific capacity, as expected from the original electrolyte (2.0 M ZnSO4 + 0.5 M MnSO4). It is hypothesized that this may be due to the fact that although the addition of H2SO4 to the electrolyte is conducive to the promotion of H+ insertion, it may not be conducive to the insertion reaction of Zn2+ so the batteries rely on the transfer of Zn2+ to release less capacity, thus limiting the capacity of the batteries, which is verified by the electrochemical tests that follow. We continued to increase the concentration of H2SO4 in the electrolyte in the hope that the batteries would provide a large amount of discharge-specific capacity during the high voltage phase of the discharge process, which could offset the decrease in the total discharge-specific capacity caused by the lower discharge capacity in the low voltage phase. As we envisioned, the discharge-specific capacity of the batteries was greatly improved when the concentration of H2SO4 in the electrolyte reached 0.1 M with good capacity retention. As shown in Fig. 2a, the discharge-specific capacity of the batteries with 2.0 M ZnSO4 + 0.5 M MnSO4 + 0.1 M H2SO4 solution as the electrolyte rapidly climbed up after a period of activation, with a more desirable activation rate. After full activation, the discharge-specific capacity of the batteries reached 536.07 mAh·g−1, and the capacity was well maintained, and the discharge-specific capacity remained at 446.57 mAh·g−1 after 100 cycles. This indicates that under appropriate acidic conditions, batteries can also provide considerable discharge-specific capacity through the chemical reaction in the high voltage phase, and this phase of the discharge reaction is often accompanied by the Mn4+/Mn2+ two-electron conversion, which has a higher theoretical specific capacity, and if we utilize this phase well, and provide a larger portion of the discharge-capacity of the battery from this phase, then we can further enhance the discharge-specific capacity of AZIBs. This phenomenon is similar to the studies by Zeng [46] and Zhong [47] and Chao [50], among others. A small portion of the capacity of the batteries decayed during the later cycles, due to the pH shift of the battery during the reaction, and as the reaction proceeds, the overall pH of the electrolyte rises so that the sulfuric acid’s effect in the electrolyte diminishes. The study by Christian [51] and his colleagues revealed the above pH change process well by adding a pH-indicating instrument to the electrolyte, which was later verified by electrochemical tests. However, when we continued to increase the concentration of the H2SO4 solution, the electrochemical performance of the batteries did not improve further, and the discharge-specific capacity of the batteries with 2.0 M ZnSO4 + 0.5 M MnSO4 + 0.2 M H2SO4 solution as the electrolyte batteries did not improve substantially in the pre-reaction period, and the specific capacity also decreased and could only reach 427.72 mAh·g−1. With the addition of 0.3 M H2SO4 solution, the electrochemical performance of the batteries was even worse, and the discharge-specific capacity could only reach 358.91 mAh·g−1, and the activation rate was even slower, with poor capacity retention and stability. This is due to the enhanced hydrogen precipitation reaction in AZIBs under more acidic conditions, which can deplete the H+ in the electrolyte and cause the pH of the electrolyte to increase, thereby affecting the electrochemical performance of the batteries. Figure 2b exhibits the GCD curves for the addition of different concentrations of H2SO4 to the electrolyte at a greater current density of 500 mA·g−1. It can be seen that the discharge-specific capacities of the batteries can reach 164.84 mAh·g−1, 225.26 mAh·g−1, 199.61 mAh·g−1, and 182.96 mAh·g−1 with the addition of 0.05, 0.1, 0.2, and 0.3 M H2SO4 solution, respectively, and the capacity change trends as well as the activation rate and other properties are similar to those at 100 mA·g−1 current density. To further test the cycling performance of these batteries after the addition of H2SO4 solution to the electrolyte, we performed the GCD test at a high current density of 1 A·g−1, and the results are shown in Fig. 2c. It can be seen that the batteries have excellent cycle life and electrochemical stability when adding 0.1 M H2SO4 solution to the electrolyte, and the discharge-specific capacity of the batteries can reach 121.57 mAh·g−1 and the capacity retention rate is 88.3% after 1000 cycles. To further investigate the effect of different concentrations of H2SO4 solution added to the electrolyte on the discharge process of the batteries, the capacity versus voltage curves of the batteries during the charging and discharging process are given in Fig. 2d. As can be seen from the figure, the discharge capacity of the batteries in the high voltage phase (1.8~1.5 V) was enhanced after the addition of H2SO4, and the difference in the capacity contribution of this phase under different concentrations of H2SO4 was not significant, which also verified the conclusion of the deepening of the discharge reaction in the high voltage phase under the acidic condition as stated earlier. Moving on to this figure, the substantial increase in capacity at 0.1 M H2SO4 compared to 0.05 M H2SO4 is mainly attributed to the capacity contribution of the chemical reaction at voltages lower than 1.5 V. This also proves that 0.1 M H2SO4 is a suitable concentration because it not only promotes the two-electron conversion reaction in the high voltage phase, but also does not interfere with the embedded detachment of Zn2+, thus increasing the batteries’ discharge-specific capacity, which also verifies the previous hypothesis. The effect of hydrogen precipitation reaction at high H2SO4 concentration can also be seen from this figure; the capacity contribution of the low voltage phase is gradually weakened as the H2SO4 concentration continues to increase from 0.1 M to 0.2 M or even 0.3 M, which is the reason for the capacity decrease at high H2SO4 concentration. In Fig. 2e, we roughly divide the discharge process of the batteries under 0.1 M H2SO4 into three stages, D1 (1.8~1.5 V), D2 (1.5~1.25 V), and D1 (1.25~1.0 V), and analyze the capacity versus voltage curves of the batteries under the addition of 0.1 M H2SO4 during the cycling process. It can be seen that the discharge capacity at each stage of the cycling process has different degrees of growth, and in the first lap of the cycle, the proportion of the capacity higher than 1.2 V to the total capacity is above 90%, and this proportion gradually decreases as the cycle proceeds, which once again confirms the conclusion that the pH of the electrolyte rises in the course of the reaction. In order to compare the changes in the charging and discharging process of the batteries before and after the addition of 0.1 M H2SO4 more intuitively, the comparative graphs of the GCD curves before and after the addition of 0.1 M H2SO4 as well as the curve of the change in the discharging capacity versus the voltage are given in Fig. 2f and g, respectively. It can be seen that the activation rate of the batteries is faster after adding 0.1 M H2SO4, and there is a substantial increase in specific capacity after 10 cycles, compared to the batteries without H2SO4 where the capacity rises substantially only after 20 cycles. In addition to this, the capacity of the batteries with 0.1 M H2SO4 added at the end of activation decays to a lesser extent, which is consistent with the previous analysis.

Fig. 2
figure 2

GCD test result image. a GCD curves at 100 mA·g−1 with the addition of different concentrations of H2SO4; b GCD curves at 500 mA·g−1 with the addition of different concentrations of H2SO4; c GCD and Coulomb efficiency curves at 1 A·g−1 with the addition of different concentrations of H2SO4; d charge-discharge capacity-voltage curves at 100 mA·g−1 with different concentrations of H2SO4 added to the electrolyte; e charge-discharge voltage curves of the electrolyte as 2M ZnSO4 + 0.5M MnSO4 + 0.1M H2SO4 during cycling; f comparison curves of GCD at 100 mA·g−1 before and after addition of 0.1 M H2SO4; g discharge capacity-voltage curve before and after adding 0.1M H2SO4

CV curves were utilized to further investigate the electrochemical performance of batteries with β-MnO2/3D GEP-CNT as the cathode material at different concentrations of H2SO4 as the electrolyte additive. The CV test results are shown in Fig. 3, where the position of each redox peak of the CV curve, the magnitude of the peak current, and the area of the CV curve correspond to the previous charge/discharge test process. The CV curves of the batteries with 2.0 M ZnSO4 + 0.5 M MnSO4 + 0.05 M H2SO4 solution as the electrolyte are given in Fig. 3a, and it can be seen that the CV curves show three reduction peaks (Peak5, Peak3, and Peak4) near 1.25 V, 1.35 V, and 1.45 V. The first two reduction peaks are consistent with those in the previous study (with 0.5M MnSO4 additive only, shown in Fig. 3i), which corresponded to the conversion reaction that produced by-products and the insertion reaction of Zn2+, respectively [49]. The oxidation peaks Peak1 and Peak2 correspond to the Zn2+ and H+ removal reactions, respectively. It is observed that, with the increase of scanning rate, the peak currents of each peak of its CV curve gradually increase, the positions of Peak1 and Peak2 move to the direction of high voltage, while Peak3, Peak4, and Peak5 move to the direction of low voltage, and the CV curves can keep similar shapes, indicating that the cathode material has good reversibility.

$$i={av}^b$$
(1)
$$\mathit{\lg}(i)= blg(v)+\mathit{\lg}(a)$$
(2)
Fig. 3
figure 3figure 3

CV test curve and their linearly fitted log(i)-log(ν) plots. a and b are the CV and log(i)-log(ν) plot with the addition of 0.05 M H2SO4; c and d are the CV and log(i)-log(ν) plot with the addition of 0.1 M H2SO4; e and f are the CV and log(i)-log(ν) plot with the addition of 0.2 M H2SO4; g and h are CV and log(i)-log(ν) plot for the addition of 0.3 M H2SO4; i and j are CV and log(i)-log(ν) plot for the addition of 0.5 M MnSO4 without H2SO4

The type of electrochemical kinetics of the cathode material can be determined by Eqs. (1) and (2) above. where a and b are variable parameters, i denotes the peak current, and v is the scan rate. a and b correspond to the intercept and slope of the linearly fitted log(i)-log(ν) plots, respectively, and when b is closer to 0.5, it indicates that the ion migration during the reaction is dominated by diffusive behavior, while when b is closer to 1, it indicates that the capacitive behavior is dominant [52]. As can be seen from Fig. 3b, the parameters b of Peak1~Peak5 are 0.73, 0.57, 0.67, 0.62, and 0.55, respectively, which are all closer to 0.5, indicating that the insertion/extraction reactions of H+ and Zn2+ are diffusion-controlled.

We continued to study the CV curves at high H2SO4 concentrations. From Fig. 3c, e, and g, it can be clearly seen that the reduction peaks corresponding to Peak5 are not obvious or even disappeared when the concentration of H2SO4 is increased to 0.1 M, 0.2 M, and 0.3 M, indicating that the provision of the discharge capacity of the batteries is dominated by the reactions corresponding to Peak3 and Peak4, and this result is in line with the results of the previous GCD test, which once again illustrates that the addition of electrolyte H2SO4 can significantly increase the capacity contribution in the discharge phase of the high voltage phase, providing batteries with higher discharge-specific capacity [53]. It is clear from Fig. 3d, f, and h that the b is still close to 0.5 at this point, again demonstrating that the electrochemical behavior of the batteries is also dominated by diffusion, which behaved consistently with no addition of sulfuric acid (as shown in Fig. 3j). The reason for the deterioration in capacity when adding H2SO4 at concentrations higher than 0.1 M can also be clued from the CV curves. As can be seen from Fig. 3e and g, compared with the CV curves at 0.1 M, the shapes of the reduction peak Peak4 in the CV curves at 0.2 M and 0.3 M do not shift much, suggesting that the insertion reaction of H+ can also be positively affected at high concentrations of H2SO4. The difference is that the peak current of the reduction peak Peak3 decreases and its shape becomes less pronounced, which suggests that the hydrogen precipitation reaction caused by the high concentration of H2SO4 in the electrolyte adversely affects the insertion of Zn2+, which is more serious at 0.3 M H2SO4, which is again in full agreement with the previous GCD test results. It is again confirmed that acidic conditions at appropriate pH are more favorable for the formation of Zn2+ and H+ co-embedded detachment mechanism to provide higher reversible specific capacity of the batteries, whereas hydrogen precipitation reaction is highly susceptible to occur under acidic conditions at lower pH, which impairs the discharge capacity and cycling stability of the batteries.

To further illustrate the embedding/de-embedding rate of Zn2+ in the batteries at different concentrations of H2SO4 as an electrolyte additive, the EIS-fitted Nyquist curves of the batteries at different concentrations of H2SO4 as electrolyte additive in the frequency range of 0.01 Hz~10 kHz as well as the Warburg impedance plots are presented in Fig. 4a and b, respectively. The rate of Zn2+ embedding/de-embedding in batteries can be reflected by the bulk-phase ion diffusion coefficient (Dion) with the following equation:

$${D}_{\mathrm{ion}}=\frac{R^2{T}^2}{2{n}^4{F}^4{A}^2{C_{ion}}^2{\sigma}^2}$$
(3)

where R is the gas constant, T is the operating temperature of the batteries (thermostat set temperature value of 298.15 K), n is the number of electrons transferred in each molecule, F is Faraday’s constant, A is the area of the electrode (1.54 cm2), and Cion is the concentration of the ions in the active substance. σ is the Warburg factor, corresponding to the slope of the Warburg impedance curve (Z′-ω−1/2) in Fig. 4b slope, and a smaller σ indicates a larger diffusion coefficient Dion. Compared with the previous study, it can be seen that the σ value when using 2.0 M ZnSO4 + 0.5 M MnSO4 + 0.1 M H2SO4 as electrolyte is only 3.59, which is smaller than when using 2M ZnSO4 + 0.5M MnSO4 as electrolyte (σ = 7.41). The σ values when adding other lower or higher concentrations of H2SO4 as an electrolyte are all larger than when using 2 M ZnSO4 + 0.5 M MnSO4 as an electrolyte alone. The calculated Dion(Zn2+) with the addition of 0.1 M H2SO4 was 1.17 × 10−11 cm2·s−1 higher than that with 2M ZnSO4 + 0.5M MnSO4 as electrolyte, which was 2.74 × 10−12 cm2·s−1 [49].

Fig. 4
figure 4

EIS test and its fitted Warburg curve. a EIS curves with the addition of different concentrations of H2SO4; b fitted Warburg curves with different concentrations of H2SO4 added

Combined with the above electrochemical performance analysis and related studies, it was demonstrated that the β-MnO2/3D GPE-CNT AZIBs complied with the H+ and Zn2+ co-insertion/extraction mechanism and successfully realized the Mn4+/Mn2+ two-electron conversion mechanism after the addition of H2SO4, with the following reaction principle:

Cathode:

$${\mathrm{Mn}\mathrm{O}}_2+4{\mathrm{H}}^{+}+2{\mathrm{e}}^{-}\leftrightarrow {\mathrm{Mn}}^{2+}+2{\mathrm{H}}_2\mathrm{O}$$
(4)
$${\mathrm{MnO}}_2+{\mathrm{H}}^{+}+{\mathrm{e}}^{-}\leftrightarrow \mathrm{MnOOH}$$
(5)
$$\mathrm{y}{\mathrm{MnO}}_2+\mathrm{x}{\mathrm{Zn}}^{2+}+2\mathrm{x}{\mathrm{e}}^{-}\leftrightarrow {\mathrm{Zn}}_{\mathrm{x}}{\left({\mathrm{MnO}}_2\right)}_{\mathrm{y}}$$
(6)

Anode:

$$\mathrm{Zn}-2{\mathrm{e}}^{-}\leftrightarrow {\mathrm{Zn}}^{2+}$$
(7)

where Eqs. (4) and (5) correspond to Mn4+/Mn2+ two-electron transitions as well as Mn4+/Mn3+ one-electron transitions, respectively. The two-electron conversion reaction of Eq. (4) takes place at the higher voltage discharge stage D1, and the one-electron conversion reaction of Eq. (5) takes place at the lower voltage D2. The electrochemical test results show that we can actually view the D1 and D2 discharge phases as a whole, and although the two-electron conversion reaction of MnO2/Mn2+ takes place in the higher voltage discharge phase, there is no clear voltage boundary between the one-electron and two-electron reactions, and the two-electron conversion is much deeper and contributes to a higher percentage of the total capacity of the discharge under the appropriate pH conditions. This view is similar to the study by Zhong [47] and his colleagues. Equation (6) corresponds to the insertion reaction of Zn2+, for which the reaction principle is also described in detail [54]. The successful construction of the Mn4+/Mn2+ two-electron conversion mechanism is actually also inextricably linked to the excellent performance of our prepared anode materials, as summarized in the following overview: (1) The lamellar structure of β-MnO2 is suitable for the insertion and detachment of H+ and Zn2+; (2) Ball milling greatly reduces the particle size of β-MnO2, which leads to a reduction in the agglomeration phenomenon, and the β-MnO2 particles are more dispersed, and the ion diffusion is accelerated; (3) The specific surface area of the cathode material increased after ball milling, and the active sites attached to the β-MnO2/3D GEP-CNT hybrid material were more easily contacted with the electrolyte; (4) The excellent performance of 3D graphene-carbon nanotubes enhanced the conductivity of the cathode material.

Considering that zinc reacts easily with sulfuric acid, we then explored the stability of the zinc anode in the electrolyte. We found from our observation experiments that in this electrolyte with a low concentration of sulfuric acid added, the consumption of zinc was not obvious, and there was no bulging of the reacted batteries, and the mass and morphology of the reacted zinc flakes did not change much compared with those without sulfuric acid added. Then, the surface characteristics of the zinc anode before and after the reaction were carefully observed with an optical microscope. Figure 5a–c are the actual pictures of anode zinc flake before reaction, after reaction without adding sulfuric acid, and after reaction with adding sulfuric acid, respectively. Correspondingly, Fig. 5d–f are the images they observed by optical microscope. There was no significant difference in the surface characteristics of the reacted zinc flakes with or without the addition of sulfuric acid. Compared to the pre-reaction period, the Zn surface showed white products and surface scratches were reduced (the scratches on the zinc flakes were caused by sandpaper polishing). This indicates that the zinc anode is relatively stable in the electrolyte used in this experiment, which is the basis for the excellent electrochemical performance of the batteries in this study.

Fig. 5
figure 5

Zinc anode sheet surface image. ac The surface of zinc anode sheet without reaction, after reaction in 2M ZnSO4+0.5M MnSO4 electrolyte and after reaction in 2M ZnSO4+0.5M MnSO4+0.3M H2SO4 electrolyte, respectively; df ac corresponding optical microscope images

Conclusion

In summary, in this paper, the prepared β-MnO2/3D GPE-CNT cathode materials were used, and H2SO4 was added to the electrolyte to regulate the electrolyte pH. Combined with XRD, SEM, TEM, XPS, specific surface area tests, and various electrochemical testing methods, we found that the excellent characteristics of the cathode materials, such as low crystallinity, minimal agglomeration, small particle size, and large specific surface area, have enabled the successful deepening of the two-electron conversion pathway of MnO2/Mn2+ by adding H2SO4 to the electrolyte. This enhancement has effectively increased the specific capacity of the batteries, resulting in batteries with good cycling stability. The results indicate that the batteries exhibit a high diffusion rate of Zn2+, an increased working potential, and a more profound level of two-electron conversion under acidic conditions conducive to a specific pH range. With 2.0 M ZnSO4 + 0.5 M MnSO4 + 0.1 M H2SO4 as the electrolyte, the batteries exhibited a reversible discharge-specific capacity of up to 536.07 mAh·g−1 at 100 mA·g−1. The activated batteries showed a reversible specific capacity of up to 85.11 mAh·g−1 even at a high current density of 1 A·g−1, with a capacity retention rate of 88.3% after 1000 cycles. This study offers an effective solution for the practical implementation of AZIBs in the power grid.