Abstract

Manganese oxide materials for high-performance supercapacitors are as popular electrode materials of energy storage devices based on their high theoretical capacitance. However, its development is limited by its poor electrical conductivity and insufficient contact surface area, which causes the supercapacitor to fail to achieve its theoretical specific capacitance. In this paper, unique sea urchin-like MnO2/biomass carbon (BC) composite materials were prepared for supercapacitors, showing the lower resistance compared with pure MnO2, which possesses superior electrochemical performance due to the advances in outstanding electrical conductivity. The single electrode test results show that the composite material achieves a specific capacitance of 205.5 F·g−1 at the current density of 0.5 A·g−1; with the current density increasing by a factor of 20, the supercapacitor loaded with this composite still retained 63.2% of its initial capacitance, showing its high rate performance. Meanwhile, the constructed asymmetric supercapacitor can change the color of electrochromic devices and drive the light of electrochemiluminescent devices, indicating its promising application. This work provided a promising route for the rational construction of multiple dimensioned high-performance electrode materials for use in new energy storage devices.

1. Introduction

With the rapid depletion of fossil fuels, the reliable and efficient conversion/storage of green energy has attracted considerable attention worldwide [16]. Compared with other energy storage devices [715], supercapacitors (SCs) have been widely used in the fields of portable electronics, heavy industry, national defense, electric vehicles, and electronic applications based on their advantages, such as high power density, rapid charge-discharge capability, and stability [1621]. In recent years, MnO2 has become the most potential material in the field of SCs due to its advantages such as low cost, high theoretical capacitance, and large voltage window in water system electrolytes [2226]. However, it is limited by the poor conductivity of manganese oxide electrode material and the instability in the cycle process, which reduces its ionic and electron transport speed and its electrochemical properties. Therefore, the development of new electrode materials for high-performance SCs still has challenges [2732].

In order to solve the problem of MnO2 used as an SC electrode, the electrochemical performance of composite carbon materials has been proven to work effectively [33, 34]. Therefore, MnO2 used for electrode materials must be combined with conductive carbon black [35], carbon nanotubes [36], graphene [37], activated carbon [38], or biocarbon [39] to improve the electrochemical energy. Biomass carbon (BC) based on pomelo peel is now a promising carbon material, which has good applications in the field of electrochemistry, catalysis, and other aspects [4046]. Using the special structure of biomass, the porous carbon material with a high-specific surface area, long cycle stability, large porosity, and good electrical conductivity can be obtained by simple carbonization and subsequent treatment. The porous carbon material combined with manganese oxide is expected to improve the electrochemical performance of manganese oxide [4450]. The introduction of biomass carbon with strong electrical conductivity can greatly increase the electrical conductivity of the whole system.

Herein, we used a simple hydrothermal method to compound the highly conductive biomass carbon prepared from pomelo skin with MnO2 nanorods to form a unique sea urchin-like MnO2/BC nanocomposite, in which the biomass carbon material with a larger specific surface area and porous structure further enables the electrochemical performance of the obtained electrode materials to meet the expectations. The specific capacitance of MnO2/BC composites’ electrode can reach 205.5 F·g−1 when the charge-discharge current density is 0.5 A·g−1. In addition, the asymmetric supercapacitor constructed by using MnO2/BC composite as the positive electrode and BC as the negative electrode maintains 105% of the initial capacitance after 4000 long cycles, showing good long-cycle stability. Therefore, the MnO2/BC composite electrode as an excellent candidate provided a promising route for high-performance SCs.

2. Experiment

2.1. Chemicals

Potassium hydroxide (KOH, 96.0%) and potassium permanganate (KMnO4, 99.5%) were purchased from Tianjin Kermel Chemical Reagent Co. Ltd. Hydrochloric acid (HCl, 37%), and ethyl alcohol (CH3CH2OH, 99.7%) was purchased from Qinhuangdao Chemical Co. Ltd. All the reagents were employed directly without further refinement. The water used throughout all experiments was purified through a Millipore system.

2.2. Preparation of Biomass Carbon

Remove the inner flesh of grapefruit peel and keep the outer skin and put it in an oven at 90°C until drying. Then, the pomelo peel is cut into smaller pieces, which are crushed in a shredder to get pomelo peel powder. A certain amount of dried pomelo peel powder was taken in a porcelain boat, and then the first precarbonization was carried out in a tubular furnace for 2 h at 700°C with a heating rate of 2°C·min−1. High-purity N2 was passed through the tube furnace at a flow rate of 50 ml·min−1. The precarbonized powder was washed repeatedly with dilute hydrochloric acid and water to remove impurity ions until pH = 7. The above centrifuged product was dried at 60°C for 10 hours. According to the mass ratio of 1 : 2, we mix a certain mass of the above samples and potassium hydroxide, and after mixing, we grind with a mortar and then mechanical ball mill for 3 hours. After ball-milling, 2 g of the mixture was placed in a porcelain boat and recarbonized at 800°C for 2 h in a tube furnace. The carbonized black powder was washed repeatedly with dilute hydrochloric acid and water to remove impurity ions until pH = 7. The above centrifuged products were dried at 60°C for 10 hours to obtain biomass carbon (BC).

2.3. Preparation of MnO2/BC Composite

Firstly, 150 mg BC was placed in 15 mL deionized water, and then a certain amount of dilute hydrochloric acid was added to BC for about 30 minutes. Then, we add 0.298 g of potassium permanganate to the above solution and stir it with a glass rod for 10 minutes until it fully dissolved. Finally, the mixture was transferred to a 20 mL reaction kettle resistant to high pressure and kept at 150°C for 12 hours. After the reaction was completed, the reaction products were removed, centrifuged, and washed with ultrapure water and ethanol at 6000 R/min, and the collected samples were placed in a drying oven and dried at 80°C for 10 hours with the mass ratio of MnO2 and BC≈1.1 : 1. In addition, we add pure manganese dioxide only without adding biomass carbon, and other steps are the same. The weight of the electrodes was all about 2 mg.

2.4. Characterization

The synthesized samples were characterized by XRD (Bruker AXS D8 diffractometer with Cu Kα radiation), SEM (JEOL JSM-840), the CHI660E electrochemical workstation, and the LAND CT2001. The battery tester was employed to measure the system with Ag/AgCl electrode and platinum sheet as the reference and counter electrode in the electrolyte of 6 M KOH aqueous solution, respectively.

2.5. Construction of Supercapacitors

The half-cell test of MnO2/BC composite material and BC electrode material in the test was completed in the system with Ag/AgCl electrode as the reference electrode, platinum sheet as the counter electrode, and active material as the working electrode. Active material, acetylene black, and teflon were mixed in an 8 : 1 : 1 ratio. Then, it spread on nickel foam as the working electrode and was pressed for 30 seconds under the pressure condition of 10 MPa and transferred to the oven after drying. In the two-electrode test, MnO2/BC composite material was used as the positive electrode and BC synthesized from pomelo skin was used as the negative electrode. The positive and negative electrode materials follow the charge balance principle The electrolyte used in the two-electrode test and three-electrode test was 1 M Na2SO4.

3. Results and Discussion

To synthesize composite electrodes, we first dried grapefruit peels and converted them into biomass carbon by carbonization. The biomass carbon obtained from grapefruit peel was activated by adding dilute hydrochloric acid and then mixed with potassium permanganate and heated hydrothermally at 150°C for 12 hours to obtain the manganese dioxide/biomass carbon (MnO2/BC) composite. In addition, pure MnO2 electrodes just do not have biomass carbon added, and all other steps are the same (Figure 1(a)). The morphologies of MnO2 and MnO2/BC composites were significantly different based on their TEM, which shows a great difference in the microstructure of the two electrode materials (Figures 1(b) and 1(c)). The pure MnO2 has a 2-dimensional wire-like structure with an average length of about 1-2 microns (Figure 1(b)). However, after compositing with biomass carbon, MnO2/BC showed a sea urchin-like structure, which is consistent with the results of transmission observation. The EDS test shows that manganese and oxygen elements are uniformly distributed in the prepared MnO2/BC composite, indicating that the MnO2 nanorods are densely distributed on the surface of BC, which may be attributed to the fact that the loose and porous carbon materials provide abundant sites for manganese oxides (Figures S1 and 1(d)).

In order to characterize the accurate structure of the MnO2/BC composite electrodes and the pure MnO2 electrodes, we provide the XRD of the electrode material before and after adding the biomass carbon (Figure 1(b)). Firstly, the XRD of MnO2 corresponds to the diffraction peak of the standard card of MnO2 (JCPDS No. 44-0141), which represents its high purity. The XRD of the MnO2/BC composites shows diffraction peaks at 12.8°, 28.8°, 37.5°, 41.9°, 49.8°, and 60.3° correspond to (110), (310), (211), (301), (411), and (521) crystal planes, respectively, indicating that MnO2/BC composites have been successfully prepared [45]. Both electrode materials show sharp peak shapes without excess miscellaneous peaks, indicating the high purity and crystallinity of the MnO2/BC electrode materials synthesized in our study. In addition, compared with pure MnO2, there is no obvious peak of biomass carbon in the diffraction peak of the composite material because the synthesized biomass carbon is amorphous.

To explore the element composition of the composite electrode material, the EDS test of MnO2/BC was conducted, which shows that manganese, oxygen, and carbon elements are uniformly distributed in the prepared MnO2/BC composite (Figure S1a). Besides, the EDS test of MnO2 shows that manganese and oxygen elements are uniformly distributed in the prepared MnO2 composite (Figure S1b). Typical N2 adsorption-desorption isotherms were supplied to further evaluate the specific surface area of the prepared MnO2/BC and pure MnO2 electrode materials [24, 29]. The data for the specific surface area in the range of 0.45–0.9 show that (Figures S2a and S2b) the MnO2/BC and pure MnO2 electrode materials have a specific surface area of 139.291 m2·g−1 and 77.301 m2·g−1, respectively, which are the typical characteristics of mesoporous materials (Table S1). The results show that in the presence of biomass carbon, the composite has a larger specific surface area than the pure MnO2 composite. The larger specific surface area of the composite can provide more active sites for electrochemical reactions. In the process of electrochemical testing, more pore structures can provide a good ion transfer pathway to supply electrolyte ions, which makes sufficient preparation for the improvement of the electrochemical performance of SC [4255].

The CV curves of MnO2/BC composite and pure MnO2 at a scanning rate of 20 mV·s−1 in the potential range 0-1 V are shown in Figure 2(a), in which both electrode materials are approximately rectangular indicating that both materials rely on the double-layer effect to store charge. In addition, the MnO2/BC electrode material exhibits a larger capacitance compared with pure MnO2 at the same scanning rate. In order to better understand the electrochemical properties exhibited by MnO2/BC, CV at different canning rates, tests were carried out under a voltage window of 0-1 V. that there is no obvious deformation of the curve as the sweep speed increases to 100 mV·s−1, indicating that the MnO2/BC electrode material has good electrochemical reversibility and stability (Figure 2(b)). The contribution of capacitance and diffusion in the MnO2/biomass carbon composite electrode is further analyzed in Figure S3. The peak current values are calculated by deriving the peak current values at different voltage scan rates after the following equation:

The b-value obtained after fitting the peak data is 0.8284 (Figure S3). Therefore, the MnO2/biomass carbon composite electrode material exhibits battery properties and pseudocapacitive properties [56, 57].

In order to further understand the electrochemical properties of the MnO2/BC electrode material, we examined the specific capacitance obtained at 0.5–10 A·g−1 (Figure 2(c)). The symmetrical charge-discharge curves indicate typical double-layer behavior. Besides, the curve still does not appear obvious voltage drop, which indicates that the resistance of the material is very small even at large current. With the current density at 0.5, 1, 2, 3, 5, 8, and 10 A·g−1, the specific capacitance of the composite material can be 205.5, 193, 176, 166, 150, and 144, respectively, while the electrochemical performance of pure manganese dioxide at the same current density is 115, 100, 90, 84, 75, 64, and 60 F·g−1 (Figure 2(d)). The MnO2/BC electrode material with biomass carbon composite exhibits better rate performance (63.2%), which retains more initial capacitance than pure manganese dioxide (52.2%).

In order to characterize the electrical conductivity of the composite material after the composite of biomass carbon, we conducted the EIS of MnO2/BC electrode material in the frequency ranging from 10−2 Hz to 105 Hz (Figure 2(e)). Both the composite material and the corresponding pure MnO2 impedance map contain two parts: a semicircle in the high-frequency region and a straight line in the low-frequency region. Local amplification of illustrations is further shown in Figure 2(e). The composite materials in the high-frequency region of the semicircle have a smaller and more steep low-frequency region of the straight line, which shows that the MnO2/BC electrode has smaller load transfer resistance, faster charge transport capacitance, and better ion diffusion ability due to a shorter ion diffusion pathway. In addition, the equivalent circuit diagram could be obtained by careful simulation of the resistance curves (the inset of Figure 2(e)), where Rs and Rct are used to represent the internal resistance and charge transfer resistance of SC, W signifies Warburg impedance, representing ion diffusion in the low-frequency region, and CPE is a constant phase angle element to simulate the capacitance properties of the electrode. Notably, the MnO2/BC electrode exhibits a higher slope line, signifying the lower diffusion resistance, indicating a faster reaction kinetic rate compared with a pure MnO2 electrode. After fitting data, the Rs and Rct values of the MnO2/BC composite electrode material were 2.23 Ω and 6.29 Ω, both smaller than those of the pure MnO2 electrode material (Table S2), which were consistent with the electrochemical experimental data. Therefore, sea urchin-like MnO2/BC composite has enhanced electrical conductivity compared with pure MnO2. To evaluate the suitability of supercapacitor materials for further practical applications, we conducted the long cycle performance test. As shown in Figure 2(f), the specific capacitance of MnO2/BC composite can still maintain 96.1% of the initial specific capacitance, which is very competitive compared with 90.4% of the pure MnO2 material at 0.5 A·g−1. The high cyclic stability indicates that MnO2 enhances the stability of the material after composite porous BC, making the electrode material more stable during continuous charging and discharging.

We used the synthesized porous biomass carbon as an anode material for supercapacitors and further characterized its morphology and electrochemical properties. The SEM diagram of biomass carbon BC shows a loose 3D network structure and large loose porous bulk structures with ordered channels, where carbon elements were evenly distributed (Figures 3(a) and 3(b)). The phase composition biomass carbon is characterized by XRD (Figure S4a), which shows two peaks, one centered around 24° with a broad and strong peak and the other around 43° with a narrow and weak peak, corresponding to the (002) and (100) crystal planes of the graphitic phase carbon of a disordered structure. The Raman test shows two distinct characteristic peaks between MnO2/BC and BC at 1309 cm−1 and 1570 cm−1, which are the characteristic D and G bands, respectively (Figure S4b). In the low-frequency range, the characteristic peak centered at 638 cm−1 is the Mn-O bond vibration, confirming the presence of MnO2 in the composite. In Raman spectra, the intensity ratio reflects the degree of the amorphous nature of the synthetic material. The higher g-band (IG) intensity in BC indicates its higher graphitized carbon, ensuring the low resistance of BC during charge and discharge [49].

The synthesized porous biomass carbon was tested electrochemically in 1 M Na2SO4 at a potential of −1-0 V., and the GCD curve of BC shows a typical double-layer charging and discharging behavior. The corresponding specific capacitance of the BC electrode material at the current density of 1, 2, 3, 5, 8, and 10 A·g−1 is 110, 100, 93, 85, 80, and 70 F·g−1, respectively (Figure 3(c)). At large magnification, there is a significant voltage drop. The curve shape did not change as the sweep speed increased from 5 mV·s−1 to 200 mV·s−1 (Figure 3(d)). Meanwhile, the impedance spectrum in the frequency range of 10−2 Hz to 105 Hz shows that the diffusion resistance (W) and charge transfer resistance (Rct) of the BC electrode material are small. The equivalent circuit diagram is further obtained based on the careful simulation of the resistance curves (the inset of Figure 3(e)), in which the Rs, Rct, and W values of the BC electrode were 1.55 Ω, 13.53 Ω, and 37.46 Ω, respectively, indicating the rapid charge transfer and ion diffusion of the biomass carbon material (Figure 3(e)). In addition, after continuous charging and discharging at 3 A/g, we found that the synthesized biomass carbon material could still maintain 100% of the initial capacitance, indicating the excellent long-cycle stability of the synthesized biomass carbon material (Figure 3(f)).

In order to evaluate the effect of MnO2/BC composite in practical application, asymmetric supercapacitors was assembled with MnO2/BC composite as the positive electrode and biomass carbon (BC) synthesized from grapefruit skin as the corresponding negative electrode. In order to determine the voltage range of the whole cell, CV tests were performed for the positive and negative electrode materials, respectively (Figure 4(a)). When the scan speed was 20 mV·s−1, the voltage range of BC and MnO2/BC composite was −1-0 V and 0-1 V, respectively. Therefore, the voltage window range of the assembled whole cell was determined to be 0–2 V. To examine the enhanced electrochemical performance after the composite biomass carbon material, CV tests performed on the whole cell composed of two electrode materials at 20 mV·s−1. Both electrode materials exhibit a rectangular shape at 20 mV·s−1. However, the full cell composed of MnO2/BC combined with biomass carbon exhibits a larger capacitance relative to pure MnO2 (Figure 4(b)). The CV test of the two electrode materials at 45–100 mV·s−1 (Figures S5a and S5b), which also presents intuitively that MnO2/BC composite has a larger capacitance than pure manganese dioxide. To detect its actual capacitance, the GCD test was carried out on the whole battery constructed by two different materials (Figure S5). When the asymmetric SCs constructed by composite materials were 0.2, 0.5, 1, 2, and 3 A·g−1, the capacities displayed were 60, 53.75, 39, 30, and 27 F·g−1, respectively. Even when the current density reaches 25 times the initial value, the specific capacitance of the whole cell can still reach 25 F·g−1, indicating the great potential of this all-cell device in practical applications (Figure 4(c)).

To distinguish the electrical conductivity of the device that can be enhanced after compound BC in the electrochemical test process, the EIS test is conducted (Figure 4(d)). The asymmetric SCs constructed by the MnO2/BC composite electrode material and BC show smaller semicircles and steeper straight lines, indicating its better ionic and electronic conductivity. To express the relationship between the energy density (E) and power density (P) of asymmetric SCs, the Ragone curve is used (Figure 4(e)). It shows that at any power density, asymmetric SCs assembled by positive and negative materials with active materials of composite BC show greater energy density. The maximum E value can reach 33.3 W·h·kg−1, even when the value is 5000 W·kg−1, and the energy density can also reach 13.9 W·h·kg−1. Such a high energy density is due to its high capacitance and 2.0 V large voltage window according to the following equation:where E represents the energy density of the asymmetric supercapacitor device, C is used to represent the capacitance that can be stored by the device, and V represents the voltage window of the entire device in the drainage electrolyte. At the same time, the power density can be calculated based on the equation (2) as follows:

Here, P stands for power density and T stands for time.

Under 0.5 A·G−1, the coulomb efficiency remains 100% even after 4000 cycles (the inset of Figure 4(f)). Besides, it can be observed that after 4000 times of continuous charging and discharging, the whole cell constructed by composite materials and biomass carbon shows better cycle stability, which can reach 105% of the initial capacitance, indicating that the electrode material obtained by composite BC shows better electrochemical performance, as compared to the recently reported supercapacitor device [5869] (Figure 4(f)).

In order to understand the performance of the full battery in practical applications, two 2.0 V asymmetric supercapacitors were connected in series and examined. The device after series still shows excellent electrochemical performance under the voltage window of 0–4 V, and the CV tests at different sweep speeds show excellent magnification performance (Figure S7a). The constant current charge and discharge test shows that the discharge time of two devices in series is twice that of one device, indicating a small capacitance loss after series (Figure S7b). Two full-cell self-assembled devices with a 4.0 V large voltage window were used to test their performance in practical applications (Figure 4(g)). It charged continuously three times at 1 A·g−1 and then connected to a red LED. The light-emitting process of the diode from bright to dark lasted for 20 minutes. Besides, we used two series of asymmetric supercapacitors to light up the pure bromoperovskite light-emitting device, which shows that the series of 4.0 V full battery could make the pure bromoperovskite from colorless to black (Figure S8). Since the asymmetric supercapacitor can combine the voltage window of the positive and negative electrodes, there are a large voltage window of 2.0 V and its own large specific capacitance. The constructed asymmetric supercapacitor shows a high energy density of 33.3 Wh·kg−1 (power density of 200 W·kg−1), which is also the reason that it can light a small bulb for 20 minutes. Three 2.0 V asymmetric supercapacitors were connected in series and used to light up a yellow electrochemical light-emitting device with Rubrene (RUB) as the light-emitting active layer, and excellent light-emitting effects were found. The excellent performance in the field of supercapacitor energy storage and perovskite discoloration gives us a reason to believe that the composite of carbon materials with high conductivity can still be an excellent solution to the problem of poor conductivity of Mn oxides.

4. Conclusions

In conclusion, we composited the porous, high-specific surface area biomass carbon material (BC) prepared by the carbonization of grapefruit peel with MnO2 and successfully prepared the anode material of high conductivity asymmetric SCs. The sea urchin-like MnO2/BC composites were achieved by the direct growth of nanorods MnO2 on the BC surface by using a simple hydrothermal method. Based on the unique sea urchin-like structure of the materials themselves, the MnO2/BC electrode material has a large specific surface area and high conductivity carbon material. The introduction of biomass carbon with strong electrical conductivity can greatly increase the electrical conductivity of the whole system. In addition, the structure combined with two-dimensional nanosheets provides more active surface, which is conducive to the enhancement of electrochemical performance. After the composite of BC, the MnO2/BC electrode material not only obtained a higher specific capacitance value compared with the pure MnO2, but also the resistance of the material became smaller. In addition, the asymmetric supercapacitor constructed from MnO2/BC positive and BC negative materials showed good long cycling ability after 4000 continuous charging and discharging cycles. The specific capacitance of the MnO2/BC composites’ electrode can reach 205.5 F·g−1 when the charge-discharge current density is 0.5 A·g−1. Considering the simple synthesis of the biomass carbon material and the excellent electrochemical performance of the obtained composite electrode materials, the method of enhancing the electrochemical performance by composite carbon materials is still attractive in the future.

Data Availability

The datasets used in this paper are available from the corresponding author upon request.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Authors’ Contributions

Xiaoyu Zhao and Ning Wang contributed equally to this work.

Acknowledgments

This work was supported by the Natural Science Foundation of Heilongjiang Province of China (No. LH2022B025), Fundamental Research Funds for the Provincial Universities of Heilongjiang Province (No. KYYWF10236190104), Natural Science Foundation of Hebei Province (No. B2020203013), and Youth Foundation of Hebei Educational Committee (No. QN2020137).

Supplementary Materials

This material is available free of charge. The EDS mapping, N2 sorption-desorption isotherms, the values of b in Logi = blogv + Log, XRD pattern, Raman spectra, full cell, the charge and discharge curve, cyclic voltammetry curves, charge-discharge diagram, the electrochromic device, specific surface area versus pore volume, equivalent circuit diagrams, and the summary of cycling stability. (Supplementary Materials)