Abstract
As an emerging energy storage device, the supercapacitor with high energy density, fast charging/discharging, and good cycle stability has aroused great interest. The performance of supercapacitors mainly depend on the electrode material. Manganese dioxide (MnO2) has emerged as one of the most promising electrode materials for high theoretical specific capacitance, wide potential range, high electrochemical activity, and environmental friendliness. However, its deteriorated volume expansion and inherently low conductivity limit its development and application in supercapacitors. To circumvent the mentioned issues, the porous, thin film, or layered composite materials were prepared to enhance the electrical conductivity and specific surface area of MnO2. Carbon materials are the ideal choice to compound with MnO2 owing to their low electrical resistance, significant thermal stability, large specific surface area, and porosity. Up to now, several kinds of MnO2/carbon composites as supercapacitor electrodes have been designed and fabricated. Herein, we give a concise review of the latest researches on MnO2/carbon supercapacitor electrodes, focusing on the fabrication strategies and analyzing the influencing factors of electrochemical performance of MnO2/carbon materials. An outlook on the possible development directions in future of designing high-performance MnO2/carbon materials for the current challenges is also provided.
Introduction
Nowadays, with the excessive consumption of traditional energy sources such as coal, oil, and natural gas, the increasingly severe global climate and deteriorating ecological environment have caused a global crisis that endangers human survival. The development and utilization of eco-friendly renewable energy become an extremely imminent task all over the world. In the past decade, solar, hydro, wind, and tidal energy and other renewable energy sources have greatly alleviated serious problems in the energy and environmental fields (Yang et al., 2011; Xie X. et al., 2019). However, abundant and clean renewable energy mentioned above cannot be widely applied directly owing to the limitation of natural conditions and the poor tunability and stability of generating electricity. Therefore, reliable electrochemical energy storage (EES), including fuel cells, ion batteries, and supercapacitors, is extremely necessary to achieve efficient storage, conversion, and further utilization of the above energy sources (Palchoudhury et al., 2019). The Ragone plots in Figure 1 shows the relationship between power density and energy density for several typical EES systems (Wang J. G. et al., 2015). Among them, electrochemical capacitors, which are also known as supercapacitors, are considered to be a new generation of green energy storage device (Díaz-Delgado and Doherty, 2016), with greater capacitance than conventional capacitors and higher output power and longer life than lithium-ion batteries (Zhang Q. Z. et al., 2018). Combined with its simple structure, high power density, fast charging, and pollution-free effects in the production process, supercapacitors are widely applied in portable electronics, data backup, hybrid electric vehicle, aerospace, and other fields (Salinas-Torres et al., 2019).
Figure 1
According to the charge storage mechanism, supercapacitors are generally classified as electrochemical double-layer capacitors (EDLCs) and pseudocapacitors (Wang G. P. et al., 2012). Energy storage and conversion of EDLCs are accomplished by static charge separation in the Helmholtz layer. Common active materials with double-layer electrodes are mostly carbon materials, which can rapidly complete the charging and discharging process and remain stable, but their capacitance and energy density are relatively low (<10 Wh kg−1) (Liang and Xin, 2015). The storage capacity of pseudocapacitors, compared with EDLCs, can be greatly improved owing to a series of reversible redox reactions on the surface/bulk phase of the electrode material (Conway, 1999). Transition metal oxides (Tajik et al., 2017) and conductive polymers (Snook et al., 2011) are commonly used as electrode materials for pseudocapacitors. The performance of supercapacitors is primarily dependent on the activity and kinetics of the electrode material. Therefore, it is very important to select suitable electrode materials, further optimize their structure, and improve their activity and kinetics to enhance the electrochemical properties of supercapacitors (Trudeau, 2013). Carbon materials and manganese dioxide (MnO2), as the most representative materials of EDLCs and pseudocapacitors, respectively, show their unique advantages in energy storage.
Carbon is one of the most closely and important elements for humans in nature and plays an important role in our existing ecosystems (Candelaria et al., 2012). It has various electronic orbital properties of sp, sp2, and sp3 hybridization, and the anisotropy of sp2 leads to various orientations of crystals and other arrays (Yu et al., 2018). Therefore, different kinds of carbon materials are formed by different chemical bonds. In particular, functional carbon materials considered to be ideal electrode materials for supercapacitors have attracted great attention owing to their low resistance, good electrical conductivity, high porosity, and large specific surface area (He et al., 2013; Borenstein et al., 2017). The EDLCs composed of carbon material form stable electric double layers by attracting mutually opposite charges at the electrode/electrolyte interface, which can achieve energy store through the physical electrostatic adsorption/desorption of charges. The energy storage mechanism is conducive to increasing the conductivity of the electrode to improve the specific capacity and energy density. Moreover, the carbon material can transform the structure and bonding mode of the composite material, thereby improving charging/discharging rate capability and cycle stability. For pure carbon materials, their specific capacitance and energy density (100~300 F g−1, 5~7 Wh kg−1) largely depends on specific surface area, porosity, and pore size distribution (Wang et al., 2019b). In recent years, a large number of functional carbon nanomaterials with related excellent properties, such as activated carbon (AC) (Faraji and Ani, 2015), graphene [including graphene oxide (GO) and reduced GO (rGO)] (Shi et al., 2018), carbon nanotubes (CNTs) (Qian et al., 2012), carbon nanofibers (CNFs) (Peng et al., 2016), and carbon aerogel (CA) (Hao et al., 2014) have emerged, which provide many favorable conditions for improving material properties. However, the specific capacitance and energy density of assembled EDLCs cannot compete with pseudocapacitors owing to their inherent electrostatic surface charging mechanism. Therefore, it is an effective way to prepare high-performance composite electrode materials by combining various functional carbon materials and typical metal oxides or conductive polymers.
Among many transition metal oxides, MnO2 with abundant reserves, low toxicity, and simple preparation process, is widely used in oxidation catalyst materials, aqueous batteries, supercapacitors, and other fields (Zhu M. et al., 2018; Li F. et al., 2019; Luo et al., 2019; Wei et al., 2019). Especially in the case of supercapacitors, MnO2 is considered to be one of the most promising electrode materials. Since Lee and Goodenough (1999) reported the pioneering work of amorphous MnO2 electrodes with excellent pseudocapacitive behavior in KCl electrolytes, a large number of efforts have been made to develop high-performance MnO2-based electrode materials. The reasons of the excellent performance of MnO2 can be summed up in two aspects. From the perspective of electrochemical properties, MnO2 displays outstanding characteristics of (a) a high theoretical capacity (1,370 F g−1) referring to the single-electron redox reaction of each manganese atom; (b) a wide potential window (0.9–1.0 V) (Xie Y. et al., 2019); and (c) excellent electrochemical properties in neutral electrolyte, leading to low chemical corrosion of the collector. From the perspective of environmental protection and economy, MnO2 is abundant in earth, has low price, and is environmentally friendly (Wei et al., 2011). These unique advantages make MnO2 an ideal choice for pseudocapacitor electrode materials. It is worth noting that MnO2 contains a variety of crystal structures, including α-, β-, γ-, δ-, and λ-MnO2; and its energy storage properties are determined by different crystal forms. Research has shown that the chain (Gao et al., 2017) or tunnel (Huang et al., 2019) structure of α-, β-, and γ-MnO2 with large two-dimensional tunneling structure facilitates electron transfer to provide a relatively high capacitance value. The large surface area of δ-MnO2 with a layered or sheet-like structure is more favorable for cation intercalation/deintercalation than the amorphous structure. The three-dimensional hinge structure of λ-MnO2 can provide more active sites for better electrochemical properties (Prélot et al., 2003; Malak-Polaczyk et al., 2010). However, the further development of current MnO2-based supercapacitors is limited by the drawbacks of MnO2 electrode materials, such as low conductivity, poor ion diffusion constant, and poor structural stability (Wang J. G. et al., 2015). Therefore, the improvement of active materials mainly involves high reversible capacitance, structural stability, and rapid cation diffusion at high charge/discharge rates. A useful and direct approach is to uniformly modify MnO2 materials onto layered porous conductive functional carbon materials to construct electrodes (Hu et al., 2018). The carbon materials can be served as a highly conductive and stable current collector, and its interconnection holes are beneficial for ion diffusion, whereas MnO2 can shorten the transmission distance of ions to prepare a high-performance electrode material.
In recent years, a large amount of significant breakthroughs have been made in the design of high-performance MnO2-based composite materials for application in supercapacitor devices. The number of research papers on MnO2/carbon composites for supercapacitors recently published is shown in Figure 2. In Figure 2a, the number of research papers on carbon/MnO2 composites has remained at a high level, which is still the research focus of electrode materials at present. And as shown in Figure 2b, recent work has shown that different types of carbon materials added to MnO2 material are mainly in forms of graphene and CNTs. This paper summarizes the synthesis strategies of MnO2/carbon materials with different morphologies and structures. The electrochemical properties and influencing factors of the electrode materials were further discussed. Finally, the remaining challenges of MnO2/carbon composite supercapacitors are briefly generalized, and an outlook on the possible development directions in the future for designing high-performance MnO2/carbon materials is also provided.
Figure 2
Synthesis And Properties of MnO2/Carbon Composites for Supercapacitor
MnO2/Carbon Nanotube Composites
CNTs are one-dimensional quantum materials with a hollow tubular structure and excellent electrical conductivity, large specific surface area, and high chemical stability (Lu et al., 2019). From the perspective of the wall structure, it can be divided into single-walled CNTs (SWCNTs) and multi-walled CNTs (MWCNTs), both of which have been widely used in the energy storage. For SWCNTs, the specific surface area can reach 240–1,250 m2 g−1, and pore size distribution is mostly in the wide range of 3 to 5 nm, with high specific capacitance of 180 F g−1, power density of 20 kW kg−1, and energy density of 6.5–7 Wh kg−1 (Fujiwara et al., 2001). And reduced electrode impedance and increased specific capacitance of SWCNTs can be obtained by the high-temperature heat treatment or addition of surfactants (Byl et al., 2005). For MWCNTs, the specific surface area (~430 m2 g−1), specific capacitance (~180 F g−1), power density (~8 kW kg−1), and energy density (~0.56 Wh kg−1) are slightly lower than those for SWCNTs (Fujiwara et al., 2001; Xie et al., 2017). In addition, carbon atoms in the CNTs are sp2 hybridized, forming a hexagonal network with the surrounding three carbon atoms, and its s orbital composition is relatively large compared with sp3 hybridization. The carbon atoms in the CNTs adopt sp2 hybridization, and the surrounding three carbon atoms form a hexagonal network, which is larger than the sp3 hybrid sulfur orbital composition. This contributed to the high mechanical strength, good flexibility, and excellent corrosion resistance and stability of CNTs that provide advantages for manufacturing flexible electrode. The introduction of carbon–carbon double bond, carboxyl group, hydroxyl group, hydrocarbon bond, and other functional groups on the surface of CNTs can improve their surface activity and help ions in electrolyte to enter into electrode materials. So far, the synthesis of CNTs has entered the commercial stage and production capacity of more than 1,000 tons (Xin and Wei, 2012). As a relatively mature nano-carbon material, the development of CNTs is of great scientific significance in the field of EES.
Considering that the specific capacitance of pure CNTs measuring 20–80 F g−1 (Dubey and Guruviah, 2019) is lower than that of other carbon materials (e.g., CNF is 120–370 F g−1 and AC is 100–300 F g−1) and acts more like a scaffold (Zhang and Zhao, 2009), scientists wisely combined MnO2 with CNTs to form nanocomposites. This composite material exerts a synergistic effect of electrical/mechanical benefits of CNTs and large pseudocapacitance of MnO2, achieving expected high specific capacity and long cycle durability. The preparation of MnO2/CNT composite electrode materials can be achieved by various synthetic methods such as electrodeposition techniques (Li Q. et al., 2014; Jeong et al., 2019), hydrothermal treatment (Ramesh et al., 2017), microwave-assisted methods (Yan et al., 2009; Li M. et al., 2017), chemical coprecipitation (Subramanian et al., 2006), and thermal decomposition (Liu et al., 2017; Bi et al., 2019). In 2006, amorphous δ-MnO2 and SWCNT composite electrode materials were first studied. As shown in Figures 3A,B, Subramanian et al. (2006) successfully prepared a δ-MnO2/SWCNT composite for supercapacitor electrodes using a simple precipitation method. Owing to the synergetic performance of double layer and pseudocapacitance, the δ-MnO2/20 wt% SWCNT composite exhibits an excellent capacitance value of 110 F g−1 at 2 A g−1 and maintains 75% capacity over 750 cycles. Further studies have found that the CNT content has a significant effect on the cycle life of the material in Figure 3C, so the reasonable ratio of CNTs and MnO2 is very critical for the electrochemical performance improvement of the composite. It is proved that the unique structure of CNTs is served as the conductive agent and support material, whereas MnO2 used as a supplier of pseudocapacitors can significantly improve the electrochemical performance of MnO2/CNT composites. This has led to a strong interest in MnO2/CNT composite electrode materials. (Li L. et al., 2019) developed MnO2-MWCNT by hydrothermal treatment directly on Ni foam for adhesive-free electrodes, as shown in Figure 3D. It can be seen from Figure 3E that ultrathin MnO2 nanosheets were uniformly grown on forest-like MWCNTs, covering the surface of the foamed nickel. The areal density, specific capacitance, and capacitance retention of the binderless electrode material prepared in this manner reached 0.775 mg cm−2, 1,350.42 F g−1 at 6.5 A g−1, and 93.9%, respectively (see Figure 3F). This derives from the direct and strong contact between the MWCNT and the current collector that achieves low charge transfer and enhances the electrochemical properties of the composites, indicating that the binderless approach can significantly improve the conductivity of the electrode material. With the great advancement of science and technology and the improvement of people's living needs, flexible and lightweight flexible electronic devices have attracted widespread attention for their soft, deformable, and easy-to-wear properties. To meet these needs, it is necessary to develop an electrode with good flexibility and excellent electrochemical performance. Wang L. et al. (2017) synthesized SWCNTs by low-crystallization hydrothermal treatment, and then mixed they with MnO2 to form an ordered network structure by vacuum filtration (see Figure 3G). The results show that the electrochemical properties of the materials can be improved by effectively regulating the regular fiber network structure. As is shown in Figures 3H,I, the area specific capacitance is 964 mF cm−2, and the capacity retention rate is 81% of the composite. The assembled hybrid supercapacitors also provide high energy densities of 31.8 μWh cm−2 at a power density of 0.815 mW cm−2, implying their great potential applications in flexible device. In addition, this review summarizes the electrochemical performance of some typical MnO2/CNT electrode materials for comparison (see Table 1).
Figure 3
Table 1
| Material | Electrolyte | Specific capacitance/F g−1 | Rate capability/F g−1 | Stability (cycles) | References |
|---|---|---|---|---|---|
| MnO2/CNT | 0.2 M Na2SO4 | 642 (10 mV s−1) | 370 (100 mV s−1) | ~70% (1,000) | Amade et al., 2011 |
| MnO2/MWCNT | 0.5 M Na2SO4 | 276 (3 A g−1) | 180.5 (9.5 A g−1) | 91.6% (5,000) | Ramesh et al., 2017 |
| MnO2/CNT sponge | 1 M Na2SO4 | 600 (1 A g−1) | 430 (10 A g−1) | ~100% (1,000) | Liu et al., 2017 |
| MnO2/MWCNT | 1 M KCl | 251 (0.5 A g−1) | – | 97% (1,000) | Subagio et al., 2019 |
| MnO2/CNT | 1 M Na2SO4 | 740 (2 mV s−1) | 503 (100 mV s−1) | 92% (1,000) | Lv et al., 2012 |
| MnO2/CNT | 0.5 M Na2SO4 | 793 (5 mV s−1) | 659 (50 mV s−1) | 97% (5,000) | Li Q. et al., 2014 |
| MnO2/CNT | 1 M Na2SO4 | 740 (10 mV s−1) | 578 (150 mV s−1) | 99.5% (800) | Fan et al., 2008a |
| MWCNT/MnO2 | 1 M Na2SO4 | 603.88 (10 mV s−1) | 405.15 (100 mV s−1) | 81% (1,000) | Li W. S. et al., 2019 |
| γ-MnO2/CNT | 0.5 M Na2SO4 | 579 (10 mV s−1) | 422 (150 mV s−1) | 87.6% (5,000) | Fan et al., 2008b |
| MnO2/CNT | 0.5 M Na2SO4 | 442.9 (2 mV s−1) | 180 (100 mV s−1) | – | Wang and Igor, 2009 |
| MnO2/CNT | 0.5 M Na2SO4 | 164 (1 A g−1) | 132 (10 A g−1) | – | Xiao et al., 2010 |
| MnO2/CNT | 0.5 M Na2SO4 | 442.9 (2 mV s−1) | 250 (100 mV s−1) | 98.9% (1,000) | Zhang et al., 2012 |
| MnO2/CNT | 0.1 M Na2SO4 | 290 (10 mV s−1) | 145 (200 mV s−1) | 88.4% (1,000) | Xin and Wei, 2012 |
| MnO2-doped PANI/CNT | 1 M H2SO4 | 1,360 (5 mV s−1) | 710 (100 mV s−1) | >82% (5,000) | Kaushal et al., 2019 |
| MnO2/SWCNT/SWCNF | 0.5 M Na2SO4 | 276 (3 A g−1) | 180.5 (9.5 A g−1) | 91.6% (5,000) | Seung Woo et al., 2010 |
| MnO2/electrospun CNT | 6 M KOH | 141.7 (5 mV s−1) | 67 (100 mV s−1) | 84.9% (1,000) | Wang N. et al., 2011 |
Electrochemical performance of various MnO2/CNT materials.
CNT, carbon nanotube; MWCNT, multi-walled CNT; PANI, polyaniline; SWCNT, single-walled CNT; SWCNF, single-walled carbon nanofiber.
MnO2/Graphene Composites
Graphene is a two-dimensional carbon nanomaterial composed of hexagonal carbon atoms in a honeycomb lattice (Huang et al., 2011; Bayle et al., 2015). With its excellent physical and chemical properties, it has shown broad application prospects in the field of energy storage and conversion (Chen P. et al., 2018; Lu et al., 2018). Interest in the study of graphene has not been attenuated after Novoselov and Geim prepared a single layer of graphene by mechanical stripping at room temperature, breaking the prediction that quasi-two-dimensional crystal materials could not exist alone at room temperature (Novoselov et al., 2004). A two-dimensional planar structure of graphene can be regarded as a building unit for constituting other dimensional carbon materials, such as zero-dimensional fullerene, one-dimensional CNTs, and three-dimensional graphite (Geim and Novoselov, 2007). In addition, the three-dimensional graphene structure can also be constructed by its self-assembling or in combination with other materials. Thanks to its two-dimensional sheet structure that can be used to construct three-dimensional electrode materials with controllable structure, it can meet the needs of no conductive agent and binder addition. The excellent electron migration rate can promote electron transport during charging/discharging to improve electrochemical performance of electrode materials. Due to the special structure of graphene, the theoretically excellent characteristics, such as large specific surface area (~2,630 m2 g−1), excellent electrical conductivity, and excellent mechanical properties (resistance). Tensile strength of 130 GPa and stiffness of 1.5 × 108 psi, and good chemical and thermal stability (Ren et al., 2018) make it a considerable industrial material that most likely to achieves scale application in the short term for EES (Kannappan et al., 2018).
However, the volumetric energy density of most graphene-based electrode materials is very low, resulting in lower energy density of the electrodes. In order to make full use of the excellent properties of graphene, adding MnO2 to graphene has become a popular choice for most researchers. This can effectively prevent graphene from agglomeration owing to strong van der Waals force by the introduction of MnO2 between the sheets (Sheng et al., 2016). And the graphene can act as carbon skeleton that exerts an “elastic constraint” to prevent electrochemical dissolution of MnO2. MnO2/graphene composites prepared by microwave irradiation, low-temperature hydrothermal treatment, in situ reduction method, and electrospinning technology have stimulated their application potential in supercapacitors or other green energy devices. Yan et al. (2010) used a fast and simple microwave radiation method to deposit nanosized MnO2 on the surface of graphene (see Figures 4A,B). The capacitance characteristics of the graphene–MnO2 composite (78 wt% of MnO2) show that the measured specific capacitance is 310 F g−1 at 2 mV s−1 (Figure 4C). This is almost three times better than that of pure graphene (104 F g−1) and birnessite MnO2 (103 F g−1). Interestingly, the weight ratio of MnO2 in the composite has a great influence on the capacitance performance. As the mass ratio increases from 20 to 78%, the specific capacitance value increases significantly. Figure 4D displays schematic preparation process of an ordered MnO2-GO fiber composite supercapacitor electrode material by electrospinning (Saha et al., 2019). The MnO2 particles with an average diameter of 260 nm uniformly distributed on the surface of graphene in Figure 4E, and the composite exhibited excellent electrochemical performance. The specific capacitance of the sample reached 863.0 F g−1 at a current density of 9 A g−1, and the specific capacitance remained 88% of the initial value after 5,000 cycles (Figure 4F). By investigating the electrochemical properties, dielectric behavior, and impedance spectra of the samples, it was found that the ordered composites have higher diffusivity and charge mobility than the disordered MnO2. It is concluded that changing the crystallinity of MnO2 with increased electrical conductivity can improve the performance of GO/MnO2 active materials. As the research progressed, ternary MnO2 composites have been widely used. For example, Zhu G. et al. (2014) anchored MnO2 nanoflakes on a graphene–CNT hybrid substrate to form a three-dimensional hybrid material without a binder (Figures 4G,H). The hybrid structure completely maintains high conductivity and high surface with increase of volume ratio of CNTs, exhibiting a capacitance value of 251 F g−1 at 1 A g−1 (see Figure 4I). A highly conductive MnO2–CNT–graphene–Ni-foamed symmetrical supercapacitor delivers an energy density of 1,200 W kg−1 at a power density of 29 Wh kg−1. It is worth noting that the crystallinity, micromorphology, and mass ratio of MnO2 in nanocomposites have a significant effect on the electrochemical performance for supercapacitors. The friendly method under mild conditions is more conducive to the shape control of MnO2/graphene and the feasibility of expanding production. Furthermore, the control of oxygen-containing functional groups and heteroatom doping of graphene is also a way to manufacture high-performance nanocomposites. The modified nanocomposite can effectively change the electronic properties of graphene and further improve the performance. In addition, this review summarizes the literature on the recently published MnO2/graphene composites in Table 2.
Figure 4
Table 2
| Material | Electrolyte | Specific capacitance/F g−1 | Rate capability/F g−1 | Stability (cycles) | References |
|---|---|---|---|---|---|
| δ-MnO2/graphene | 1 M Na2SO4 | 270 (0.5 A g−1) | 168 (15 A g−1) | 90.12% (50,000) | Wang et al., 2019a |
| MnO2/graphene | 1 M KOH | 342.8 (0.5 A g−1) | 111.2 (20 A g−1) | 90.3% (3,000) | Wang H. et al., 2019 |
| N-doped graphene/MnO2 | 1 M Na2SO4 | 411.5 (0.5 A g−1) | 242 (20 A g−1) | 88.3% (4,000) | Le et al., 2019 |
| MnO2/GO | 1 M Na2SO4 | 315 (0.5 A g−1) | – | ~95% (5,000) | Wu et al., 2010 |
| MnO2/GO | 1 M Na2SO4 | 360.3 (0.5 A g−1) | 223.6 (5 A g−1) | >93% (1,000) | Dai et al., 2014 |
| MnO2/rGO | 1 M Na2SO4 | 759 (2 A g−1) | 196 (50 A g−1) | 88% (3,000) | Jadhav et al., 2019 |
| MnO2/rGO | 1 M Na2SO4 | 234.8 (0.1 A g−1) | 136.9 (5 A g−1) | 100% (10,000) | Chen Y. et al., 2018 |
| MnO2/graphene | 1 M Na2SO4 | 255 (0.5 A g−1) | – | 84.5% (10,000) | Zhang Q. et al., 2019 |
| MnO2/graphene | 1 M Na2SO4 | 133 (10 mV s−1) | 104 (150 mV s−1) | 75% (10,000) | Amade et al., 2019 |
| Graphene/MnO2/CNTs | 1 M Na2SO4 | 372 (0.5 A g−1) | 194 (10 A g−1) | >90% (3,000) | Cheng et al., 2012 |
| Sponge@rGO@MnO2 | 1 M Na2SO4 | 205 (0.1 A g−1) | 136.9 (5 A g−1) | 90% (20,000) | Ge et al., 2013 |
Electrochemical performance of various MnO2/graphene materials.
GO, graphene oxide; rGO, reduced GO; CNTs, carbon nanotubes.
MnO2/Carbon Nanofiber Composites
CNFs are a type of carbon material that is internally composed of a layer of graphite carbon oriented along the fiber axis. According to different precursors of raw silk, CNFs are mainly divided into three classifications: polyacrylonitrile (PAN)-based carbon fiber, pitch-based carbon fiber, and rayon carbon fiber (Wazir and Kakakhel, 2009). Compared with AC materials, carbon fiber has obvious advantages in performance. The connection of the large, medium, and large number of small holes on the surface is very favorable for the transport of the electrolyte and the adsorption of the charges. Moreover, the excellent heat resistance, low thermal expansion, chemical stability, and good electrical conductivity make them very suitable as electrode materials for supercapacitors (Kim et al., 2019). Generally, CNFs can be prepared by chemical vapor deposition (CVD) and spinning, using carbon ammonia compounds (including methyl, hexyl, ethyl, and carbon monoxide) as carbon precursors. The ammonium bicarbonate molecules are decomposed at high temperatures under the catalysis of metal catalysts such as iron, diamond, and ruthenium; and carbon atoms diffuse into the graphite layer to form a fibrous structure. The spinning method extrudes the precursor polymer into multiple continuous filaments through wet spinning, gel spinning, baking–melting, dry spinning, and electrostatic spinning, among which electrostatic spinning technology is the most widely applied (Zhang et al., 2015).
Owing to the compact structure, low porosity, and small specific surface area (<10 m2 g−1) of CNFs in practical applications (Sun et al., 2018), using pure CNFs as electrode materials leads to poor electrochemical performance. Therefore, they can be used as a substrate-carrying MnO2 pseudocapacitor material to improve the electrochemical activity of the electrode, thereby preparing a high-performance composite electrode. Zhao H. et al. (2016) obtained bubble CNFs by exploding PAN at temperatures of 1,000°C in Figure 5A. The electrode after decoration with MnO2 nanosheets has a capacitance value of 428 F g−1 at 1 A g−1 owing to the easy electron transport path of CNFs (Figures 5B,C). After 1,500 cycles, the specific capacitance of composites still remained 98.8%. Ma et al. (2016) used electrospun lignin-derived high-graphite electrospun CNF (ECNF; ~200 nm in diameter and ~583 m2 g−1 of specific surface area) as the substrate and then decorated with MnO2 nanowhiskers to obtain three kinds of nanocomposites with different weight percentages of MnO2 (Figure 5D). The electrochemical performance of the sample with a mass ratio of ECNF and MnO2 of 1:1 is optimal. The supercapacitor device prepared by using the composite as an electrode material has a specific capacitance of 83.3 F g−1, an energy density of 84.3 Wh kg−1, and a power density of 5.72 kW kg−1 (Figures 5E,F). As shown in Figure 5G, an effective solar technology was reported by Zhao C. et al. (2017). They successfully recovered regenerated carbon fiber (RCF) from carbon fiber-reinforced polymer (CFRP), and then the α-MnO2 nanowires were uniformly grown on the surface of the high temperature-treated RCF. The MnO2/RCF composite (MRCF) prepared by processing CNF at 150°C has an extremely large potential window (1.6 V) and excellent electrochemical performance (specific capacitance is 228.8 F g−1 at 1 A g−1, and high cycle stability is ~91.2% after 3,000 cycles) in Figures 5H,I. The asymmetric supercapacitor assembled with the composite as the positive electrode has an operating potential window of 2.0 V and exhibits a high energy density of 22.9 Wh kg−1. There are relatively few studies on MnO2/CNF, and some of the results are shown in Table 3. It is found that rationally designing the microstructure of MnO2/CNF composites and enhancing the electrochemical utilization of MnO2 can effectively improve EES.
Figure 5
Table 3
| Material | Electrolyte | Specific capacitance/F g−1 | Rate capability/F g−1 | Stability (cycles) | References |
|---|---|---|---|---|---|
| CNF/MnO2 | 1 M HCl | 311 (2 mV s−1) | 159 (200 mV s−1) | 97.6% (1,000) | Zhi et al., 2012 |
| CNF/MnO2 | 6 M KOH | 142 (10 mV s−1) | – | – | Nataraj et al., 2013 |
| MnO2/catalytically grown CNF | 1 M Na2SO4 | 257 (5 mV s−1) | – | 105% (1,000) | Zhou et al., 2017 |
| CNFs/MnO2 | 0.1 M Na2SO4 | 557 (1 A g−1) | 186 (30 A g−1) | 94% (1,500) | Wang J. G et al., 2011 |
| CNFs/MnO2 | 0.5 M Na2SO4 | 365 (1 A g−1) | – | 95.3% (1,000) | Wang et al., 2013 |
| MnO2/CNF | 0.1 M Na2SO4 | 374 (2 mV s−1) | 198 (100 mV s−1) | 94% (1,000) | Wang J. G. et al., 2012 |
| CNT/CNF/MnO2 | 1 M Na2SO4 | 517 (5 mV s−1) | – | 75% (1,000) | Wang T. et al., 2015 |
Electrochemical performance of various MnO2/CNF material.
CNF, carbon nanofiber.
MnO2/Activated Carbon Composites
AC is a carbon material prepared by pyrolysis and activation of carbon-containing raw materials such as wood, coal, and petroleum coke. It has developed pore structure, large specific surface area, and abundant surface chemical groups (Abioye and Ani, 2015). According to the pore size, it can be classified into three types: macropores (≥50 nm), mesopores (2–50 nm), and micropores (≤ 2 nm) (Wei et al., 2016). In the energy storage mechanism, large pores are usually used as ion buffers, mesopores (transition pores) are used for efficient ion diffusion, and micropores are used to store charges. Owing to the rich pore structure of AC, its specific surface area can reach up to 3,000 m2 g−1 (Barbieri et al., 2005), which creates favorable conditions for charge storage. AC possesses characteristics of stable chemical properties, abundant sources, wide operating temperature range, simple preparation process, large specific surface area, and environmental protection (Wang Y. et al., 2019). It has been considered to be the most extensive electric double-layer electrode active material in commercial applications. AC for electrodes of electric double-layer capacitors is usually derived from nature, such as charcoal, husks, and biomass, and can also be obtained by carbonized polymers. Generally, the synthesis process of AC is to carbonize a carbonaceous organic precursor in an inert atmosphere at a high temperature and then activate the carbon materials having a high specific surface area by physical or chemical activation. Physical activation is usually performed by injecting CO2 or water vapor at high temperatures to the system, followed by removing precursor uncarbonized substances and selective oxidation of carbides (López Ch et al., 2015). KOH, ZnCl2, and H3PO4 are usually used as activators for chemical methods with carbonized substances to selectively react to form pores and increase specific surface (Abioye and Ani, 2015). According to the double-layer capacitance theory, the specific capacitance of AC is greatly affected by the specific surface area. The initial research hopes to increase specific capacitance by expanding specific surface area and pore volume of carbon materials. However, it is found that the capacitance of electrode materials is not linearly related to the specific surface area. Even if the specific surface area increases a lot, the increase of specific capacitance is still limited. Moreover, these shortcomings will in turn reduce the energy density and power density of AC electrode.
In order to further obtain high energy density and volume density, typical pseudocapacitive materials such as MnO2 are increasingly anchored on AC to obtain ideal electrode materials. Chen M. D. et al. (2014) selected cotton stalk as carbon precursor and synthesized an amorphous AC material with 1,481 m2 g−1 of specific surface area using H3PO4 as activator by one-step chemical activation. After that, electrolytic MnO2/AC composites with different contents of MnO2 were prepared, as shown in Figure 6A. The galvanostatic charge test confirmed that the composite with 5% MnO2 (labeled as AC4) has optimum specific capacitance (169 F g−1) and excellent cycle life (99.2% after 500 cycles), as shown in Figures 6B,C. With the deepening research, Zhang J. et al. (2019) proposed a novel high-voltage anode electrodeposition technique to deposit graded MnO2 on AC cloth (Figure 6D). Interestingly, it was found that the AC cloth was activated to have a significant improvement in the conductivity and hydrophilicity of the composite electrode. It can be seen from Figure 6E that benefiting from the high conductivity of the closely contacted AC cloth/MnO2 interface, the electrode exhibits a specific capacitance of 400 F g−1 in 1 M of Na2SO4 at 0.5 A g−1 in an asymmetric supercapacitor, and the impressive volumetric energy density reaches 3.82 mWh cm−3. Figure 6F shows the good flexibility and mechanical properties of the composite. In Figures 6G,H, Li H. et al. (2019) combine AC fibers with MnO2 to form electrodes with excellent flexibility and excellent capacitance properties. The area ratio of the composite material is as high as 410 mF cm−2, delivering a high energy density of 36 μWh cm−2 and a high power density of 726 μW cm−2 (Figure 6I). Integrated devices with multiple electrodes can successfully illuminate light-emitting diodes, showing great potential applications. Finally, it is found that the perfect pore structure and proper surface modification that can function as a fast transfer ion and increase the wettability of the electrode surface are beneficial for suitable pore size distribution. Moreover, the presence of the AC can prevent agglomeration of MnO2 and maximize the MnO2 pseudocapacitance. Table 4 summarizes the electrochemical performance of some representative MnO2/AC composites. It shows that MnO2/AC composites, as an environmentally friendly supercapacitor electrode material, have become a preferred choice for researchers.
Figure 6
Table 4
| Material | Electrolyte | Specific capacitance/F g−1 | Rate capability/F g−1 | Stability (cycles) | References |
|---|---|---|---|---|---|
| AC/MnO2 | 6 M KOH | 193 (0.2 A g−1) | 154 (2 A g−1) | 77.8% (1,500) | Liu et al., 2015 |
| Porous AC/MnO2 | 6 M KOH | 258 (1 A g−1) | 235 (20 A g−1) | 93.6% (10,000) | Kong et al., 2019 |
| MnO2/AC cloth | 1 M Na2SO4 | 257 (5 mV s−1) | – | 94.2% (5,000) | Shen et al., 2019 |
| AC/MnO2 | 1 M Na2SO4 | 297.8 (0.2 A g−1) | 155 (20 A g−1) | 94.8% (1,000) | Kim et al., 2015 |
| AC/MnO2 | 1 M Na2SO4 | 90.5 (5 mV s−1) | – | 91.3% (1,000) | Kim et al., 2013 |
| MnO2/spherical AC | 0.1 M Na2SO4 | 357 (1 A g−1) | – | 93% (3,000) | Li Z. et al., 2014 |
Electrochemical performance of various MnO2/CNT material.
CNF, carbon nanofiber; AC, activated carbon.
Summary and Outlook
This review summarizes the research achievements in synthesis methods and electrochemical performance of MnO2/carbon composites for supercapacitors in recent years. In this system, MnO2 provides a source of high specific capacitance and high energy density, while carbon materials ensure excellent cycle performance and high power density. Impressively, various functional carbon materials exhibit their own excellent physical and chemical properties in different dimensions, which provides feasibility to rationally optimize the microstructure and maximization of electrochemical properties of MnO2/carbon electrode materials. Among these carbon substrates, one-dimensional carbon materials of CNTs and CNFs can provide high-speed diffusion and shorten ion diffusion paths owing to their high conductivity and good mechanical properties, becoming the preferred choice for flexible supercapacitors. Two-dimensional carbon materials represented by graphene are regarded as ideal conductive substrates for their high specific surface area, ultra-low density, and good electrical conductivity. Other AC materials with typical three-dimensional structure are widely used in preparing energy storage devices with high energy density due to their large number of microporous structures and rich functional groups. In general, carbon nanomaterial with excellent porous structure and high conductivity can maximize the electrochemical performance of MnO2. Orderly and tidy channels (such as mesoporous carbon) can accelerate the transport of electrolyte ions and make it easier to enter MnO2. Meanwhile, enhancing the degree of graphitization of carbon materials (such as CNTs and graphene) is conducive to the improvement of conductivity to ensure rapid transfer of charge. In recent years, numerous efforts have been made to explore high-performance MnO2/carbon composites for supercapacitors, and exciting improvements have been achieved. However, there are still remaining several key drawbacks in those composites, such as the lack of ordered pore channels in the carbon substrate (Wang T. et al., 2015), the violent volume expansion and low electrochemical utilization rate of MnO2 (Lei et al., 2012; Sun et al., 2017), and optimization of the composite structure (Zhang Q. Z. et al., 2018).
Faced with these practical challenges and obstacles, we believe that much more efforts should be focused on developing new-generation MnO2/carbon composites that can better meet the energy storage requirements and standards of advanced supercapacitors in the future. Therefore, we suggest that future research trends may focus on the following aspects:
(1) For MnO2/CNTs or CNFs, a carbon substrate with the optimal pore size distribution and specific surface area should be constructed to increase the specific capacity and power density of the supercapacitor; improve the poor surface wettability of CNTs by surface modification, ultrasound, and other treatments to ensure uniformity of MnO2 deposition; and optimize the design of flexible and foldable CNF substrates that meet different requirements without sacrificing stable power output and long cycle stability.
(2) For MnO2/AC, the low-mass load problem of MnO2 should be improved without sacrificing the power of the composite material to balance the overall performance, effectively exerting the coordination performance of MnO2 and carbon materials.
(3) For MnO2/graphene, MnO2 should be deposited more uniformly on the surface of graphene and should establish an intimate connection by the new composite technology to prevent the damage of composite structure and improve the rate capability and cycle stability.
(4) MnO2 should be combined with economical and green carbon materials to develop light, low-price, and environmentally friendly composite electrode materials.
Statements
Author contributions
All authors listed have made a substantial, direct and intellectual contribution to the work, and approved it for publication.
Funding
This work was supported by research program of the Key Laboratory for Biomedical Effects of Nanomaterials and Nanosafety, Chinese Academy of Sciences (NSKF201908).
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Nomenclature
| Acronyms | Full name |
|---|---|
| AC | Activated carbon |
| B-CNFs | Bubble carbon nanofibers |
| CA | Carbon aerogel |
| CFRP | Carbon fiber-reinforced polymer |
| CNFs | Carbon nanofibers |
| CNTs | Carbon nanotubes |
| CVD | Chemical vapor deposition |
| ECNF | Electrospun carbon nanofiber |
| EDLCs | Electrochemical double-layer capacitors |
| EDS | Energy-dispersive X-ray spectroscopy |
| EES | Electrochemical energy storage |
| GO | Graphene oxide |
| MnO2 | Manganese dioxide |
| MRCF | MnO2/regenerated carbon fiber |
| MWCNTs | Multi-walled carbon nanotubes |
| PAN | Polyacrylonitrile |
| PEG | Polyethylene glycol |
| PVA | Polyvinyl alcohol |
| RCF | Regenerated carbon fiber |
| rGO | Reduced graphene oxide |
| SDS | Sodium dodecyl sulfate |
| SWCNTs | Single-walled carbon nanotubes |
| ZnO NPs | ZnO nanoparticles |
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Summary
Keywords
MnO2, carbon materials, composites, electrode material, supercapacitor
Citation
Wu D, Xie X, Zhang Y, Zhang D, Du W, Zhang X and Wang B (2020) MnO2/Carbon Composites for Supercapacitor: Synthesis and Electrochemical Performance. Front. Mater. 7:2. doi: 10.3389/fmats.2020.00002
Received
28 September 2019
Accepted
06 January 2020
Published
11 February 2020
Volume
7 - 2020
Edited by
M. Jasim Uddin, University of Texas Rio Grande Valley Edinburg, United States
Reviewed by
Minshen Zhu, Leibniz-Institut für Festkörper- und Werkstoffforschung (IFW Dresden), Germany; Aminur Rashid Chowdhury, University of Texas at Austin, United States
Updates
Copyright
© 2020 Wu, Xie, Zhang, Zhang, Du, Zhang and Wang.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Wei Du duwei@ytu.edu.cnXiaoyu Zhang zhangxiaoyu@ytu.edu.cn
This article was submitted to Carbon-Based Materials, a section of the journal Frontiers in Materials
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