Du Huang,
Zhenya Lu*,
Qian Xu,
Xingyue Liu,
Wenbin Yi,
Junning Gao,
Zhiwu Chen,
Xin Wang and
Xiaoyi Fu
School of Materials Science and Engineering, South China University of Technology, Guangzhou 510641, China. E-mail: zhylu@scut.edu.cn
First published on 24th June 2021
A nano-porous Al/Au skeleton is constructed to effectively improve the utilization rate of the active MnO2 and the overall adhesion between the current collector and MnO2 in an electrodeposition system. The Al/Au current collector is prepared by first forming a nano-porous structure on the surface of Al foil through etching modification, and subsequently coating an ultra-thin Au layer onto the Al foil. The active MnO2 is electrodeposited on the Al/Au current collector to fabricate a novel Al/Au/MnO2 electrode. The nano-porous skeleton supports MnO2 to grow autonomously inside-out. The ultra-thin Au layer acts as a transition layer to improve the overall conductivity of the current collector (0.35 Ω m−1) and to improve the adhesion with MnO2 as well. Owing to the highly porous structure, the electrochemical properties of the electrode are greatly improved, as evidenced by a remarkable specific capacitance of 222.13 mF cm−2 at 0.2 mA cm−2 and excellent rate capability of 63% capacitance retention at 6.0 mA cm−2. Furthermore, the assembled solid-state symmetric supercapacitor exhibits a high energy density of 0.68 mW h cm−3, excellent cyclic stability (86.3% capacitance retention after 2000 cycles), and prominent flexibility.
A typical supercapacitor is generally composed of active material and a current collector, electrolyte, and separator. It is well acknowledged that the active materials provide energy storage capacity for supercapacitors. Therefore, in order to obtain electrodes with high specific capacitance, researchers put effort to grow various nanostructured active materials with high specific surface area (Sa), such as nanotubes, nanospheres, and nanoflowers, etc.6–11 However, the synthesis methods for these structures are rather complicated, time-consuming. In fact, as the carrier for active materials, current collector is also a particularly crucial component, because the intrinsic characteristics of which determine the application scenarios of supercapacitors. In addition, some pseudocapacitive active materials with poor conductivity must be attached to the current collector to transmit electrons. Therefore, an ideal current collector should have high conductivity, strong adhesion with active materials, and good supporting stress. Common current collector materials include conductive metal (aluminum foil, copper foil, etc.), metal foam (foam nickel, foam aluminum, etc.), carbon substrate (carbon cloth, carbon paper, etc.) and some other conductive substrates. However, it is unfavorable to employ pristine metal substrate as current collector to support a mass of active materials, because the Sa of pristine metal is generally too low for insufficient contact area with the active material.12 Besides, the carbon cloth and the nickel foam are much more expensive than the metal foil. Thus, finding superior current collector materials remains challenging. Portet et al.13 reported a modification method of Al current collector that exhibited great surface contact and interface conductivity (0.4 Ω cm−2) between the carbon nanofibers. Huang et al.14 used picosecond laser scanning to construct hierarchical micro-nano patterned surface of Al current collector to increase surface area. Lang et al.15 developed a nano-porous gold current collector to support the growth of nanocrystalline MnO2, showing an extremely high specific capacitance. Meng et al.16 synthesized a polypyrrole (PPy)-decorated nano-porous gold (NPG) electrode with high volumetric capacitance. Kim et al.17 constructed a porous and oriented NiO–TiO2 nanotube arrays electrode by electrochemically anodizing Ni–Ti alloy foils. These methods were designed to prepare porous and high Sa current collectors for more active materials to grow, leading to improved specific capacitance. Another factor worth considering is the adhesion between current collector and active materials, for which affects the electrochemical performance and cyclic stability of supercapacitors. Kim et al.18 and Wang et al.19 discovered that coating graphene onto Cu and Al current collectors could better protect them from corrosion while improving the electrochemical properties, cyclic stability, and interlayer adhesion. It is therefore can be summarized that, from the perspective of perfecting the current collector, the performance of supercapacitor can be improved via (1) increasing its Sa; (2) enhancing its conductivity and adhesion with active materials.
On the other hand, electronic devices are developing into the direction of flexibility and portability, so the research on flexible supercapacitors has also attracted much attention.20 The key to flexible supercapacitors is the flexible current collector and solid electrolyte.21 Aluminum (Al) foil is an ideal current collector material due to its high conductivity, good flexibility, stable mechanics and more importantly, low cost. Generally, there are two typical etching processes to increase the Sa of Al foil. The first option submerges the Al foil into the acid solution (chemical etching).13 The secondary option is electrolysis where the Al as the anode is placed in acid solution to form porous Al2O3 (AAO) layer (electrochemical etching).22 However, the preparation process for AAO is usually time and energy consuming. In overall consideration on the preparation process complexity, acid etching is chosen in this investigation. In previous works, researchers usually grew carbon-based materials on Al current collector to form double layer supercapacitor, but the specific capacitance of such electrodes only realized to ∼100 F g−1.13,14 In order to achieve a higher specific capacitance, transition metal oxide MnO2 was chosen to grow onto the Al current collector to prepare pseudocapacitive capacitors in this work. Electrodeposition is a common method of growing thin films, which has the advantages of simple, convenient and one-step operation. However, so far, no reports have been found about directly depositing MnO2 onto Al current collector by electrodeposition method. This may be due to the poor adhesion of Al itself or the aluminum oxide thin surface layer formed by oxidation of Al foil with MnO2 in the electrolyte of electrodeposition system. The specific mechanism is still unknown. Kavian et al.23 grew MWCNT felt onto Al foil first and then electrodeposited MnO2 to form composite electrode. However, the Al foil in the report was flat type which only acted as a role in transporting electrons. The MnO2 actually grown upon the CNT framework. It was also strange that in the control experiment, nickel sheets were selected to be current collector for electrodepositing MnO2 but not the original Al foil. So, maybe a transition layer was needed to grow onto the Al foil to enhance the overall adhesion between current collector and MnO2 if the electrodeposition was conducted.
In this work, the optimal conditions to form nano-porous structure of Al foil by etching modification were explored. In order to both utilize the nano-porous structure and the conductive property of etched Al foil, a large amount of coating and electrodeposition experiments had been explored, and we finally found that the adhesion between gold (Au) and Al or MnO2 was both good. Thereby, an ultra-thin Au layer was coated onto the Al foil to obtain Al/Au current collector. Then, the MnO2 could be successfully electrodeposited onto the Al/Au skeleton to form an Al/Au/MnO2 electrode. The nano-porous skeleton could support massive MnO2 to grow inside-out autonomously. Compared with the electrode prepared by pristine Al foil, the modified electrode exhibited superior electrochemical properties with a much higher specific capacitance, enhanced rate capability and better cyclic stability. Moreover, based on the Al/Au/MnO2 electrodes, the assembled symmetric solid-state supercapacitor presented excellent flexibility, high energy and power density.
The areal capacitance (CA, F cm−2) of the electrodes and supercapacitors derived from CV and GCD are evaluated by eqn (1) and (2), respectively,
![]() | (1) |
![]() | (2) |
The volumetric energy density (E, mW h cm−3) and power densities (P, mW cm−3) of the supercapacitors are evaluated by eqn (3) and (4), respectively,
![]() | (3) |
![]() | (4) |
Fig. 2e displays the XRD patterns of A3/Au current collector and AAM3 electrode. It is obvious that all the diffraction peaks of A3/Au current collector can be indexed to Al (JCDPS 89-2769). Nevertheless, none of the peaks corresponds to manganese oxide, suggesting that the MnO2 prepared by electrodeposition is amorphous in nature which is consistent with previous report.24 Raman spectra of AAM3 electrode (Fig. 2f) exhibits peaks at 575 cm−1 accorded with Mn–O bond in the MnO6 octahedral and 638 cm−1 accorded with the Mn–O bond of the MnO2 framework,25 which also confirms the successful preparation of MnO2.
The specific surface areas of all the samples are measured by N2 adsorption and desorption test and shown in Fig. 2g. The curves correspond to a typical IV isotherm hysteresis loops.26 According to the BET analysis, the pristine Al foil exhibits a relatively small Sa of 0.044 m2 g−1. After etching modification, the Sa of A3 foil increase by nearly 40 times to 1.654 m2 g−1. When the ultra-thin Au layer is coated onto the A3 foil, the Sa can maintain 1.564 m2 g−1, which verify that the ultra-thin Au layer do not sacrifice the high Sa of nano-porous substrate. The AAM3 electrode presents a higher Sa of 7.301 m2 g−1. The pore size distribution (Fig. 2h) indicates the mesopores ranging from 2 to 8 nm of A3 foil and AAM3 electrode, which mainly attributes to the pores of current collector and the numerous gaps between MnO2 nanowires.
The XPS spectrums in Fig. 3 show the chemical states and composition of the AAM3 electrode. The XPS survey spectrum of the electrode indicates the existence elements of Au, Mn and O (Fig. 3a) which is consistent with the EDS results. The high-resolution Mn 2p spectrum (Fig. 3b) presents two obvious peaks at 642.2 and 653.8 eV, corresponding to Mn 2p3/2 and Mn 2p1/2 of Mn4+, agreeing with the previously reported MnO2 value.27,28 The high-resolution O 1s spectrum (Fig. 3c) presents three different peaks at 529.7, 531.1 and 532.4 eV, corresponding to Mn–O–Mn,29 Mn–O–H and water (H–O–H).30 Two peaks at 83.7 and 87.43 eV (Fig. 3d) corresponds to Au 4f7/2 and Au 4f5/2 core levels, respectively.31
The above analyses reveal the growing process and the uniform distribution of MnO2 from the nano-pores to the surface of the modified A3/Au current collector, also confirm the successful synthesis of nanoscale MnO2.
As the AAM3 electrode presents the largest CV loop and CA among the obtained electrodes, the properties of AAM3 are further investigated in detail. Fig. 4b shows the CV curves of AAM3 measured from 5 mV s−1 to 100 mV s−1. The current density increases with scan rate. CV curves under low scan rates (5, 10, 25 mV s−1) present symmetric quasi-rectangular shapes without redox peaks, demonstrating the excellent storage characteristic and reversible pseudo-capacitance. The electrode tends to show a certain resistance behaviour and slightly deviates from the quasi-rectangular shapes at high scan rates (50, 100 mV s−1) due to the inefficient contact between MnO2 and electrolyte ions at high scan rates. In addition, the CV performance of electrodes obtained under different deposition voltages and times base on the A3/Au current collector are also investigate (Fig. S6†). It is found that the initial voltage that MnO2 can be successfully deposited onto the current collector is about 0.5 V, and deposition is hard to proceed for the voltage below this value. When the deposition voltage exceeds 0.8 V or the deposition time exceeds 400 s to further increase the mass loading of MnO2, the specific capacitance decreases instead. This phenomenon can be explained by the excessive MnO2 forming a thick layer that seals the nano-pores of the A3/Au current collector and prevents the internal MnO2 from effectively contacting the electrolyte, which retard the function of the porous structure.15
The rate capability of the AAM3 electrode is further investigated by GCD measurement with various current densities from 0.2 mA cm−2 to 6 mA cm−2 at a 0–0.8 V potential window (Fig. 4c). The GCD curves present nearly symmetric triangular shapes, showing the excellent electrochemical capacitance characteristics of AAM3 electrode. Besides, all GCD curves show well linearity in the relationship between potential and time, demonstrating the sufficient and reversible reaction between the MnO2 in electrode and the alkali ion (Na+) in electrolyte. The relationship between CA and scan rate or current density is shown in Fig. 4d. The highest CA calculated by CV curves achieves 219.3 mF cm−2 at 5 mV s−1, then gradually descends to 100.25 mF cm−2 at 100 mV s−1. The highest CA evaluated by GCD curves achieves 222.13 mF cm−2 at 0.2 mA cm−2 or 302.9 F g−1 at 0.27 A g−1 (in order to compare with the Al/carbon electrode mentioned above). At low current density (0.2, 0.4 and 0.6 mA cm−2), the ions in the electrolyte can access and contact with almost all available active sites of MnO2, performing a complete insert-reaction and leading to high CA. However, this effective interaction between and MnO2 and electrolyte ions is hard to proceed thoroughly when increasing the current density, thus causing the reduction in CA. Nevertheless, even the current density is expanded by 30 times to 6 mA cm−2, the CA can still maintain 139.5 mF cm−2, with a 63% retention, indicating excellent rate capability and rapid charge–discharge process. The excellent rate capability can be attributed to the nano-porous structure of metal/oxide electrode, in which nanoscale MnO2 grows along the internal pores and rough surface of highly conductive A3/Au current collector, allowing electrons to contact with electrolyte ions easily and efficiently to provide fast redox reaction even under a high current density. As shown in Table 1, the CA of the AAM3 electrode is higher than comparable to the previous results of MnO2-based electrode. Unlike those MnO2-based electrodes mentioned in literatures, we start from the perspective of modification of Al/Au current collector, a relatively high specific capacitance can also be obtained without constructing complex multilayer structure or using expensive carbon-based materials or templates. It is believed that the AAM3 electrode stores charge by both the surface adsorption/desorption of Na+ cations and the reversible, and rapid MnO2 redox reaction (Mn4+/Mn3+) on the surface and interior of the electrode according to eqn (5) and (6).4,43
![]() | (5) |
![]() | (6) |
Electrodes | Electrolyte | Specific capacitance (mF cm−2) | Operating voltage (V) | Ref. |
---|---|---|---|---|
MnO2/ZnO | 1 M Na2SO4 | 230 at 10 mV s−1 | 0.8 | 11 |
MnO2@AuNF | 1 M Na2SO4 | 8.26 at 5 mV s−1 | 0.8 | 34 |
Ni/rGO/MnO2 | 1 M Na2SO4 | 119.4 at 0.5 mA cm−2 | 0.8 | 35 |
α-Fe2O3/MnOx | 1 M Na2SO4 | 227 at 0.5 mA cm−2 | 1.0 | 36 |
AgQDs/MnO2 | 1 M Na2SO4 | 97.4 at 0.02 mA cm−2 | 0.8 | 37 |
H-ZnO/MnO2 | 0.5 M Na2SO4 | 138.7 at 1 mA cm−2 | 0.8 | 38 |
FeOOH/MnO2 | 1 M LiClO4 | 252 at 1 mA cm−2 | 0.8 | 39 |
H-MnO2/CC | 0.5 M Na2SO4 | 220 at 0.75 mA cm−2 | 0.8 | 40 |
MnO2 NWs | 5 M LiCl | 150 at 1 mA cm-2 | 0.8 | 41 |
CNPs/MnO2 | 0.1 M Na2SO4 | 109 at 5 mV s−1 | 0.8 | 42 |
AAM3 | 1 M Na2SO4 | 222.13 at 0.2 mA cm−2 or 219.3 at 5 mV s−1 | 0.8 | This work |
The frequency response and the conductivity of the AAM3 electrode are demonstrated by EIS measurement ranging from the frequency of 0.01 Hz to 100 kHz. Fig. 4e shows the Nyquist plots of the AAM3 electrode and the inset gives the equivalent circuit, in which Rs, Cdl, Rct, Zw and CL represents the intrinsic internal resistance,44 the double layer capacitance, the faradic charge-transfer resistance, the Warburg impedance, and the limit capacitance,45 respectively. The impedance spectrum exhibits a semicircle shape in the high frequency region and a straight line in the low frequency region. Rs and Rct obtained from the high frequency region are about 3.26 Ω and 1.72 Ω, respectively, demonstrating the low internal and charge-transfer resistance due to the highly conductive A3/Au current collector. The slope of 45° portion of the curve reflects the Zw of the electrode, representing fast ions diffusion from the electrolyte to the electrode.37 In addition, the straight line with a large slope in low frequency region indicates the ideal capacitance performance. The above results from Nyquist plots confirm the improved conductivity of coating Au layer upon A3 foil and the good adhesion between the current collector and MnO2, thus leading to the rapid ions diffusion/transportation ability at the interface of electrolyte/electrode and in the bulk electrode. Although MnO2 has inherently low conductivity which restricts its charge–discharge rate,46 the charge transfer reaction pseudocapacitance of the AAM3 electrode can be enhanced by rapid ions diffusion in the three-dimensional nano-porous current collector and through the highly conductive framework of the A3/Au foil as well as the metal/oxide interface.
The cyclic stability (Fig. 4f) of AAM3 is evaluated by GCD measurement for 2000 cycles under a current density of 3 mA cm−2. After cycling, the CA of AAM3 decreases from 147 mF cm−2 to 125.25 mF cm−2, with 85.2% retention, showing prominent cyclic charge–discharge stability. It is observed that little MnO2 detach from the A3/Au current collector. The porous structure of A3/Au current collector can well withstand the volume expansion and contraction of MnO2 caused by cyclic charging and charging. The surface SEM images of the electrode after cycling is presented in Fig. S8.† It is found that the structure of MnO2 changes from nanowire to nanosheet after 2000 cycles (Fig. S8a and b†), leading to the decrease of specific capacitance. The AAM electrode prepared by the pristine Al/Au foil shows poor stability in the cyclic GCD test (Fig. S8c†), and CA only remains 59.5% after 1000 cycles of test. After cyclic test, the MnO2 nanowires also convert to nanosheets, while some MnO2 film can be observed to delaminate from the Al/Au current collector (Fig. S8d†). This indicates that the MnO2 grows upon planar structure is easy to shed off when the volume changes, thereby leading to the degradation of CA and poor stability.
The Ragone plots (Fig. 5f) reveal the relationship between volumetric energy and power density of the assembled supercapacitor. The supercapacitor exhibits a maximum energy density of 0.68 mW h cm−3 at a power density of 5.33 mW cm−3, and a highest power density of 53.33 mW cm−3. These values exceed or are comparable to some previously reported symmetric systems based on MnO2, such as H-ZnO2/MnO2 (0.04 mW h cm−3),38 FeOOH/MnO2 (0.05 mW h cm−3),39 MnO2/CNPs (0.05 mW h cm−3)42 and some MnO2-based asymmetric supercapacitors, such as H-TiO2/MnO2//H-TiO2/C (0.30 mW h cm−3),9 ZnO/MnO2//r-GO (0.234 mW h cm−3),11 α-Fe2O3/C//α-Fe2O3/MnOx (0.64 mW h cm−3),36 H-MnO2//RGO (0.25 mW h cm−3),40 α-Fe2O3 NTs//MnO2 NRs (0.55 mW h cm−3),41 N-Fe2O3//MnO2 (0.41 mW h cm−3)47 and MnO2/graphene//VOS@C (0.95 mW h cm−3).48 Moreover, based on the nano-porous current collector, different active materials can be grown to assemble into asymmetric supercapacitor, thus widening the charge–discharge voltage window and leading to significantly enhanced energy density. Further research is on the way.
Fig. 6a shows the schematic drawing of the supercapacitor with a sandwich structure and the physical drawing of three supercapacitors connected in series. Furthermore, the flexibility of supercapacitor is demonstrated by CV measurement (Fig. 6b) under different bending states (from 0° to 180°) at the same scan rate of 50 mV s−1. Under different bending angles, the CV curves can well maintain the original quasi-rectangular shape with little change of capacity, indicating good mechanical stability of the device which can ascribe to the excellent flexibility of the Al current collector. The current collectors with qualified supportive capacity, flexibility and stability enable the supercapacitors have further possibilities in applications, such as micro and flexible electronic devices, which fully demonstrates the vital role of current collector in supercapacitors. In order to verify the practical value of the supercapacitor, three supercapacitors are connected in series firstly and then charged with two AA batteries for several seconds, then a commercial red LED light can be lit up under different bending states for a while (Fig. 6c). A switch is also added into the circuit, the supercapacitor after charging is used as the power source to control the LED on and off. The LED can response rapidly, which confirms the excellent stability and switching characteristic of the fabricated supercapacitors. The evidenced video is attached in the ESI.†
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra01923f |
This journal is © The Royal Society of Chemistry 2021 |