Md. Mahinur Islam,
M. Yousuf Ali Mollah,
Md. Abu Bin Hasan Susan and
Md. Mominul Islam*
Department of Chemistry, Faculty of Science, University of Dhaka, Dhaka 1000, Bangladesh. E-mail: mominul@du.ac.bd
First published on 21st December 2020
α-MnO2 has been recognized as a potential material for supercapacitor applications because of its abundance, cost-effectiveness, environmental-benign nature and high theoretical specific capacitance (Csp) of 1370 F g−1. In this study, we succeeded for the first time to achieve the theoretical Csp with 3D multi-walled carbon nanotubes (MWCNTs) horizontally dispersed on 2D graphene oxide (GO) nanosheet framework-supported MnO2 ternary nanocomposites synthesized by a simple precipitation method. The in situ formation of α-MnO2 and GO, and the growth of 3D MWCNT/GO framework took place simultaneously in a strong acidic suspension containing functionalized-MWCNTs, graphite, NaNO3 and KMnO4. Characterizations of the composites synthesized by varying % wt MWCNTs were performed with state-of-the-art techniques. These composites were characterized to be semi-crystalline and mesoporous in nature, and the scrupulous analyses of field emission scanning electron microscopic images showed MnO2 nano-flower distributed over 3D MWCNTs dispersed-on-GO-nanosheet frameworks. These composites deposited on a graphite electrode exhibited an ideal supercapacitive behavior in an Na2SO4 solution measured via cyclic voltammetry and chronopotentiometry. Optimum contents of MnO2 and MWCNTs in the composites showed a maximum Csp of 1380 F g−1 with satisfactory energy and power densities compared in the Ragone plot. An ascending trend of Csp against the charge–discharge cycle number studied for 700 cycles was noticed. Well-dispersion of α-MnO2 nanoparticles throughout 3D MWCNTs covalently-anchored to the GO nanosheet framework is discussed to aid in achieving the frontier Csp of MnO2.
The high prospect of the α form of MnO2 in designing supercapacitor electrodes has been focused because of its high theoretical Csp of 1370 F g−1.13 The experimentalists in this field are in a kind of race to reach this milestone of theoretical Csp by attempting to tune the morphology of MnO2 using mainly carbonaceous and polymeric frameworks. Accordingly, huge numbers of research works have been published in recent years on this focal issue.14,15 The research work on MnO2 as a supercapacitor material has been launched from the work of Lee and John in 1999.16 The amorphous MnO2·H2O has been reported to show a Csp of 200 F g−1 in an aqueous KCl solution.16 Later on Liu et al. achieved a Csp of 379 F g−1 by tuning the morphology of MnO2 to form a bowl-like nanosheet with an ultra-thin thickness (ca. 4 nm) synthesized by a template-assisted hydrothermal method.15 Wang et al. have shown the influence of electrolytic media on the Csp of Mn3O4-embedded-graphene composite to be 175 F g−1 in 1.0 M Na2SO4 and 256 F g−1 in 6.0 M KOH solutions.17 It has been revealed that Csp decreases drastically as the thickness of the MnO2 film increases.13 This is reasonable since the underlying part of the nonporous material would not play the role in the charging-discharging cycle to contribute to Csp.
Recently, Huang et al. have pointed out several crucial points in fostering Csp of materials including the use of highly conductive, porous and conductive polymeric materials as the dispersing matrix.15 The researchers have succeeded to some extent by following these routes in designing efficient MnO2 composites with different frameworks to enhance Csp to, e.g., 242 F g−1 with MnO2/polyaniline (PAni) composites,18 300 F g−1 with an in situ electrodeposited PAni/MnO2 composite,19 395 F g−1 with MnO2/PAni/multi-walled carbon nanotubes (MWCNTs) composites,20 646 F g−1 with stalagmite MnO2 nanorod arrays growing vertically on flexible Ni substrates,21 752 mA h g−1 with MnO2–graphene having a sandwich structure22 and 964 F g−1 with multi-layered graphene/CNTs/MnO2 nanocomposite inter-connected pore networks.23 As far as we reviewed, the study by Jia et al. is the latest, wherein the highest Csp of MnO2 of 1229 F g−1 has been achieved by creating a special tube-on-sheet architecture of the meso-structured composite of CNT-on-MnO2 nanosheets of which the CNTs are vertically aligned on porous MnO2 nanosheets.24 This study has in fact motivated us in using MWCNTs covalently fixed on graphene oxide (GO) nanosheets as the dispersing agents for MnO2.
MWCNTs is an attractive material used in numerous applications including as a filler owing to its good electrical conductivity, high surface area, mechanical strength, chemical stability and low mass density.25,26 MWCNT itself does not meet the requirements for a commercial storage devices due to its low Csp only of 58 F g−1.27 The low Csp probably arises from the high aggregation of MWCNTs via strong hydrophobic forces that results in a poor exposure of the active site to the electrolytes.26,28 On the other hand, GO is a 2D material derived from graphite by introducing covalent C–O bonds first reported in 1855.29 Due to its ability to remain exfoliated in water as single atomic-layered sheets, cast as films, and be further reduced back to graphene, GO has been used in numerous applications as conductive films, electrode materials and composites.29
In this study, we successfully synthesized efficient ternary composites of MnO2/MWCNTs/GO by following basically two-fold molecular engineering as: (i) the dispersion of MWCNTs via the formation of an ester-like bond between the –COOH group of functionalized MWCNTs and the –OH group of GO and (ii) the dispersion of in situ formed nanoparticles of MnO2 via a precipitation method over the MWCNT/GO matrix formed simultaneously. Prior to the formation of composites, the introduction of the –COOH group on the MWCNT surface was carried out by a strong acid treatment.30 Binary composites of MnO2/GO were also prepared. The as-prepared composites were characterized with Fourier-transform infrared (FTIR) spectroscopy, field emission scanning electron microscopy (FESEM), energy dispersive X-ray spectroscopy (EDS), X-ray diffraction (XRD) and Brunauer–Emmett–Teller (BET) surface analysis techniques. The storage characteristics of the composites deposited on graphite electrodes were evaluated via cyclic voltammetry and galvanostatic charge–discharge (GCD) measurements.
Materials synthesized/treateda | Abbreviated name | % MnO2 contentb | BET characterizations | |||
---|---|---|---|---|---|---|
Surface area (m2 g−1) | Pore diameter (nm) | Mean pore diameter (nm) | Total pore volume (cm3 g−1) | |||
a % represents feed amount of MWCNT.b Determined with EDS. | ||||||
Graphene oxide | GO | — | — | — | — | — |
GO/MnO2 | GOM | 2.50 | 4 | 1.48 | 4 | 0.004 |
Functionalized MWCNT | F-MWCNT | — | 105 | 37.03 | 50 | 1.315 |
5% MWCNT + GO/MnO2 | GMCNT-5 | 0.52 | 7 | 1.86 | 12 | 0.035 |
10% MWCNT + GO/MnO2 | GMCNT-10 | — | 15 | 2.12 | 19 | 0.045 |
15% MWCNT + GO/MnO2 | GMCNT-15 | 0.75 | 14 | 2.55 | 24 | 0.085 |
30% MWCNT + GO/MnO2 | GMCNT-30 | 0.65 | 12 | 2.20 | 20 | 0.056 |
50% MWCNT + GO/MnO2 | GMCNT-50 | 0.15 | 7 | 2.29 | 14 | 0.025 |
It formed a long-standing dispersion. The thus-formed negatively charged –COOH group would repeal each other and did not allow the MWCNTs to aggregate, as in the case of pristine ones. The chemical reaction involving the formation of the ternary composite of 3D MWCNT-top-on-GO nanosheet frameworks is expressed in ESI.† The in situ formation of α-MnO2 and GO, and the growth of the 3D MWCNT/GO framework through the reaction between –OH groups of nascent GO formed instantly and –COOH groups of F-MWCNT added in a suspension containing graphite, NaNO3 and KMnO4 occur simultaneously under strong acidic conditions (Scheme 1). The binary composite of MnO2/GO was prepared in the absence of F-MWCNT.32 These materials were subjected to relevant characterizations and used to modify graphite electrodes used as supercapacitor electrodes.
The introduction of –COOH groups on MWCNT surfaces was successful as confirmed by FTIR spectral analyses (Fig. 1a). The two characteristic bands at 1720 and 2350 cm−1 are associated with the stretching vibrations of >CO and O–CO groups, respectively, of the –COOH group.35–37 The bands at 1410 and 1227 cm−1 correspond to the O–H deformation and stretching vibration of C–O, respectively, confirming the presence of the epoxy group.38 A strong, broad band at 1590 cm−1 for the aromatic CC group, confirms the presence of sp2 hybridized carbon in GO (Fig. 1b).38 Moreover, a sharp peak at 615 cm−1 for Mn–O vibration39,40 with the characteristic epoxy bands at 1405 and 1250 cm−1 for GO were also observed. The weak band at 1060 cm−1 indicates the C–OH stretching vibration of the alkoxy group for GOM composites.41–43 Thus, these oxygen-containing functional groups indicate that the graphite is oxidized to form GO.44
In the FTIR response typically shown for GMCNT-15, several characteristics features are noticed: (i) the blue shifts of >CO (1728 cm−1) and the alkoxy C–OH (1076 cm−1) group of F-MWCNT, (ii) diminishing of the bands around 3450, 1450 and 1250 cm−1 associated with O–H vibration, O–H deformation, C–O epoxy stretching of chemisorbed water, respectively.38 The observed blue-shift of the band of the >CO group confirms the formation of an ester-linkage in the composite.45 The decrease in the intensity of the broad band between 3600 and 3000 cm−1 is indicative of the removal of chemisorbed water in GMCNT-15 through H-bonding as the OC–O bond is formed.38 The possibility of these reactions can be further supported by the studies of Jorden et al. and Luckhaus et al., where hydrogen-bonding interactions between GO and with F-MWCNT have been modelled theoretically.46,47 The extent of interactions depends on the efficiency of the insertion of F-MWCNT between the GO sheets during the in situ exfoliation process, best achieved at 15% of F-MWCNT. Thus, the –COOH group of F-MWCNT reacts with the –OH group of GO to form an ester-like linkage in this acidic environment.45 The FTIR spectra of other GMCNT composites are described in ESI.†
In the typical EDS response of GMCNT-15 (Fig. 2f), the characteristic peaks of Mn, C and O elements were observed. The % mass of these elements were determined by spotting on three distinct positions of the FESEM image. Similar studies for all binary and ternary composites were carried out and the values of % MnO2 are summarized in Table 1. The % MnO2 in GOM is 2.50, i.e., GOM contains about 97% of C and O species as GO. In general, the ternary composites contain a small amount of MnO2, among which GMCNT-15 contains the highest % MnO2 of 0.75. The growth of MnO2 would simultaneously take place on the surface of GO and MWCNT and inside the pores of MWCNTs, i.e., in situ formed MnO2 fills the tube of MWCNTs. Although it is not clear, the underlying MnO2 in the ternary composite including MWCNT-30 and MWCNT-50 may not be exposed for detection with EDS. Consequently, the amount of MnO2 loading was observed to decrease upon increasing the amount of MWCNTs in the ternary composite.
Fig. 2 FESEM images of (a) GOM, (b) F-MWCNT, (c) GMCNT-15, (d) GMCNT-30 and (e) GMCNT-50, and (f) typical EDS spectrum of GMCNT-15. |
Fig. 2 illustrates FESEM images of the as-prepared materials. In the low magnification image of the GOM composite, GO nanosheets are found to be curly separated with a number amount of MnO2 nanoparticles densely deposited on their layer. The high magnification FESEM image shown in the inset clearly shows the nano-flower morphology of MnO2 particles (Fig. 2a). The FESEM image of F-MWCNT shows that MWCNTs are highly coagulated and bundled, whereas F-MWCNTs are distributed quite uniformly and MnO2 are dispersed on MWCNT and GO sheet in GMCNT-15. MWCNTs were found to reform aggregates in GMCNT-50 as in the case of F-MWCNT. The particle size distribution with the particle count of all GMCNTs, which were statistically evaluated by measuring the diameters of 100 randomly picked nanoparticles is shown in ESI.† GMCNT-15 has the highest particle counts with an average size of 10.30 nm. In GMCNT-50, there is a significant reduction in the particle count with a simultaneous increase in the average area of the particles. From these observations, it can be inferred that the functionalization of MWCNT is an effective method for preventing their agglomeration, and GO-assisted well-dispersion of MWCNTs up to their certain compositions and in situ formed MnO2 particles are uniformly distributed over the binary bed of the MWCNT/GO framework in the ternary composites.
Fig. 3 represents the XRD patterns of the GMCNT composites. The sharp peak at 2θ of 26.0° is a characteristic of the (002) plane of MWCNTs.48 The characteristic peak of GO was found at 2θ = 11.9° with an interlayer distance of 0.83 nm.43 The peaks observed at 42.3 and 56.4° with a low intensity correspond to the (101) and (201) planes of α-MnO2.21,49 A decrease in the intensity is observed and the peak becomes broader as the amount of MWCNTs increases. It is worth mentioning that the shape, size and crystal planes of crystallite affect the shape of diffraction patterns (for details see ESI†). However, the crystallinity of GMCNT-5 was determined to be 90% with 13.5 nm single crystal of MWCNTs. Their degree of crystallinity and the size of crystallite decreased to become amorphous with a decrease in the feed amount of F-MWCNTs (see Table SI-1†). Most remarkably, the GMCNT-15 composite is only 17% crystalline with the crystallite size of 0.22 nm. The amorphous parts of the composite that has been reported to favour the electrolyte to insert into or to expel out from the matrix50 during the charge–discharge cycle are beneficial to increase Csp (vide infra).
As shown in Fig. SI-5,† the experimental XRD patterns of the sample matched well with the stimulated pattern of the triclinic crystal system with the P1 space group. The microstructure of the composite exhibits patterns of the oxide layer with Mn and C bridge adjacent layer into 3D architectures (Fig. SI-6†).51 Thus, the as-synthesized 3D architectures are entirely made up of randomly oriented and entangled MWCNTs with amorphous GO and in situ formed α-MnO2, as depicted in Scheme 1. Multi-covalent junctions of MWCNT such as Y-junctions were found within the entangled network structure.52 The MWCNT inter-linked with GO and in situ MnO2 via esterification by the epoxy matrix formation in the presence of a strong acid,31,53 which can be confirmed by the degree of dispersion.
The N2 gas adsorption–desorption isotherms of the composites are shown in Fig. 4. The hysteresis loop is similar to the H3 type of mesoporous materials.45,54 The BJH plots exhibit the distribution of the pore diameter. The surface parameters determined for all materials are summarized in Table 1. F-MWCNTs naturally possesses a high surface area of 105 m2 g−1 with a large pore diameter of 37 nm. Both surface area and pore diameter of MWCNTs anchored to GO nanosheets significantly decreased in the presence of MnO2 due to the disperson of MnO2 occurring not only on the surface but also inside the pores of MWCNT. It is interesting to note that when in situ formed MnO2 in the GMCNT composites was maximum the surface and pore diameter became maximum (see Table 1). For GMCNT-15, i.e., at the optimum composition of MWCNTs and MnO2, the pore diameter was maximum, which is important for the charging-discharging of a material (vide infra).
Fig. 4 Nitrogen adsorption–desorption isotherms of (a) GMCNT-5, (b) GMCNT-10, (c) GMCNT-15 and (d) GMCNT-50 composites. Inset represents corresponding BJH plots. |
Fig. 6 shows GCD responses measured by applying constant current densities ranging from 0.5 to 20 A g−1. The observation of the symmetrical GCD response demonstrates a high reversibility between the charging and discharging processes, as observed in the case of CV studies. The increasing current density shortens the charging time as a consequence of a lower degree of alignment/insertion of solvated Na+ ions at/into the surfaces of materials forming a double layer. Ideally a longer charging time allows a high degree of insertion of solvated ions in the pore of the material, thus forming a rigid double layer.56 The discharging time of the GCD response was used to calculate the Csp as compared in Fig. 7.
Fig. 7 Comparison of the specific capacitance of different materials under consideration. Csp values of MnO2 (theoretical),13 MWCNTs26 and GO59 were taken from the literature. |
Fig. 7 illustrates the comparison of the experimental values of Csp for F-MWCNTs, GOM and GMCNTs with the theoretical value of α-MnO2. At a glance, GMCNT-15 exhibited an excellent supercapacitive behaviour with the Csp of 1380 F g−1. With the increasing amount of F-MWCNTs in the ternary composite, Csp increased initially and then decreased owing to a further increase in the % F-MWCNTs. It is rather interesting to note that Csp varies in a convex parabolic fashion against the feed amount of F-MWCNTs. The Csp of individual F-MWCNT is excessively low,26 while that of GOM binary composites was 400 F g−1 in agreement with literature.33 The combination of GOM and 5% F-MWCNTs in the GMCNT composite slightly enhanced Csp to 420 F g−1. An increase in Csp was observed by increasing the percentage of F-MWCNTs up to 15% and then Csp showed a decreasing trend in against further increase in F-MWCNTs. Csp decreased with an increase in the current density applied for the GCD measurement and the amount of material loaded (see ESI†). This decrease in Csp is due to the scarcity of the effective contact between the active surface on the electrode and electrolyte ion.56
The underlying reasons associated with frontier Csp of MnO2 obtained experimentally can easily be explained by considering the % MnO2 present and the surface characteristics of GMCNT composites as described above. MWCNT itself provides a low Csp, though it possesses a large surface area and high porosity. Pristine F-MWCNTs and GO show a purely double layer charging.26,57 Conversely, the charging of MnO2 involves a surface chemisorption of electrolyte ions, i.e., Na+ (eqn (1)), resulting in pseudo-capacitance. The charging-discharging cycle involves the rapid intercalation and de-intercalation of Na+ ions, leading to the reduction and oxidation of MnO2.13 During charging-discharging, the conversion of Mn(III) to Mn(IV)13,57 has been considered for graphene–MnO2 (ref. 33) and GO–MnO2 composites.57
MnO2(s) + Na+(aq) + e− ⇌ MnOONa(s) | (1) |
The extent of charging and hence Csp generally depends on the amount of the accessible surface for the electrolyte ions and the amorphous nature of the oxide materials. The highly amorphous structure favours the electrolyte to insert into or to expel out from the oxide matrix.58,59 On the contrary, the active surface area and ion-permeable porosity are the keys to regulate the ion accessible surface area. The size of hydrated ions of an aqueous electrolyte is in the range of 0.60–0.76 nm. Therefore, the micropores are not suitable for the insertion of hydrated ions due to the screening effect. However, the examination of data of % MnO2 present that surface area, pore size, pore volume and degree of crystallinity GMCNT-15 possesses all the prerequisite features of an ideal supercapacitor material at their optimized levels. A moderate pore size (>2) nm is needed to maximize the electrical double layer capacitance by easy mobility and insertion of individual electrolyte ions into pores of the carbon electrodes.59 However, the pores of more than 7 nm are not suitable for the adsorption of inserted ions since they loosely bind and hence do not form a compact double layer.58,59 The surface of GMCNT-15 containing thin array of MnO2 nanoparticles with suitable pores may function for the permeation of electrolyte ions in a lock and key manner that regulates enhanced effective ion diffusion via the nano-structure-top-on GO sheets for charging-discharging through the redox reaction, as shown in eqn (1).57
The long-term cyclic stability of GMCNT-15 was tested for 700 cycles (Fig. 8). Csp was found to increase with the cycle number. Cheng et al. have also observed this increase for MnO2 and this process is known as electro-activation.33 Upon continuous cycling, the GO sheets may move to adjust to different electrolyte ions.33 The long-time charging-discharging may also help the ions access fully the sheets of GMCNTs to extract a full advantage of the surface area. The GMCNT-15 modified hybrid electrode exhibited a high energy density of 94.6 W h kg−1 and power density of 200 W kg−1 that are derived from the GCD measurement. The Ragone plot illustrated in Fig. 8 clearly shows that GMCNT-15 can store higher energy compared to lithium-ion batteries and supercapacitors, although being pseudocapacitive in nature, it possesses lower power density than a typical electric double layer capacitor.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0ra08772f |
This journal is © The Royal Society of Chemistry 2020 |