Nanostructured Manganese Dioxide for Hybrid Supercapacitor Electrodes

Abstract

Hybrid supercapacitors, as emerging energy storage devices, have gained much attention in recent years due to their high energy density, fast charge/discharge and long cyclabilities. Among the wide range of systems covered by this topic, low cost, environmental friendliness and high power provide MnO₂ with great characteristics to be a competitive candidate. The present work reports a hybrid aqueous supercapacitor system using a commercial activated carbon as the negative electrode and a synthesized manganese dioxide as the positive electrode. Two manganese dioxide polymorphs (α-MnO₂ and δ-MnO₂) were tested in different neutral and basic aqueous electrolytes. In this way, full cell systems that reached an energy density of 15.6 Wh kg⁻¹ at a power density of 1 kW kg⁻¹ were achieved. The electrode–electrolyte combination explored in this study exhibits excellent performance without losing capacity after 5000 charge/discharge cycles, leading to a promising approach towards more sustainable, high-performance energy storage systems.

1. Introduction

One of the most critical challenges to overcoming the increasing environmental problems as well as the fast consumption of coal, gas and oil, is the deployment of ecological and consistent energy sources. However, renewable energy sources do not produce energy around the clock; thus, to be effectively utilized they require cheap, sustainable and efficient energy storage technologies [1,2]. For the above reasons, energy storage systems are a hot topic at the moment, attracting the attention of very varied fields of science, and benefiting from innovative techniques and multiple approaches to improve them [3,4]. Although most of the attention is focused on the use of batteries, especially lithium-ion batteries, but also electrochemical capacitors or supercapacitors (SCs), other emerging technologies such as sodium-ion batteries also need to be considered in this pool. Due to their fast charge and discharge rates, high power density and long-term cycling stability, SCs can be effectively combined with batteries, or even replace them, to design a custom-made solution [5,6]. These properties make SCs widely used devices in electric vehicles, military equipment, uninterruptible power supplies and many other applications that require high power input [7,8,9].

Based on the working mechanism of the electrodes, SCs can be classified in two main categories: electrical double-layer capacitors (EDLCs) and pseudocapacitors (PCs). The former rely on the electrosorption of electrolyte ions on the surface of the electrode to accumulate charge in the electrode–electrolyte interface [10]. Therefore, EDLC electrodes are generally made of carbon-based materials because of their large specific surface area (SSA), excellent electrical conductivity, and good electrochemical and mechanical stability [11,12,13]. Activated carbons (ACs) are usually selected due to their high porosity and large SSA (~1000–2500 m² g⁻¹) [14,15,16,17]. However, it is known that large surface area does not always translate into high capacitance values, and ultimately, energy, but pore size also plays an important role [18,19,20]. Nevertheless, despite their high specific power and long lifetime, the specific energy of EDLCs is limited by the lack of bulk charge storage (10–300 F g⁻¹) [21,22].

On the other hand, PCs undergo fast and reversible Faradaic redox reactions that occur on the electrode surface during cycling [23,24,25]. Yet, when switching to PCs the reaction kinetics are slower and the electrical conductivity is lower, which translates into lower power output. Therefore, pseudocapacitors are usually focused to work at higher capacitances but in slightly higher charge/discharge times [26,27]. The PCs are generally fabricated using transition metal oxides (TMOs) and hydroxides such as Ni(OH)₂, V₂O₅, Co₃O₄, NiO, Co(OH)₂, etc., due to the ease of synthesizing them as nanoparticles, leading to a high porosity and SSA, and their ability to change between more than one oxidation state [28,29,30,31,32]. RuO₂ has been widely studied because it possesses one of the highest electronic conductivity and theoretical capacitance of around 1450 F g⁻¹ [33]. However, as it is quite non-abundant and expensive, researchers have been studying alternative compounds [34].

Among all of the candidates, MnO₂ has proven to be one of the most promising materials because it is cheap, non-toxic, abundant and it also has a high theoretical specific capacitance (1370 F g⁻¹) [35]. Contrary to other pseudocapacitive systems such as Co₃O₄ or NiO, in aqueous electrolyte MnO₂ shows a full working potential window of ~1 V, achieving higher energy densities [36]. Nonetheless, as in other TMOs, due to its low conductivity (10⁻⁷–10⁻³ S cm⁻¹), the capacitance becomes greatly reduced with increasing mass of the electrode, leading to practical values of ~250 F g⁻¹ [36,37,38,39,40]. However, the implementation of high conductive additives such as Au, carbonaceous materials or conductive polymers, can successfully overcome this problem [41,42,43]. Other approaches have also been tested in order to deal with the poor conductivity of this material. Nanostructuring the electrodes is one of these promising methods because it produces a larger electrode–electrolyte interface, which enhances surface charge storage and it also obviates the low conductivity because of the short diffusion pathways of the nanostructure [24].

MnO₂ can be easily synthesized in different polymorphs with different electrochemical performances. Some of the most remarkable ones are α-, β-, and γ-MnO_2, in which the electron transfer is facilitated by its two-dimensional tunneling structure. The layered structure of δ-MnO₂ favours the cation intercalation/deintercalation processes, giving rise to an excellent performance as an electrode material [24,44]. Reactions for surface and bulk charge storage are shown in Equations (1) and (2), respectively [28,45,46]:

(MnO₂)_surface + A⁺ + e⁻ ↔ MnOOA_surface

(1)

MnO₂ + A⁺ + e⁻ ↔ MnOOA

(2)

where ${\mathrm{A}}^{+}={\mathrm{Li}}^{+},{ \mathrm{Na}}^{+},{ \mathrm{K}}^{+},$ etc. Another way to deal with the low conductivity of MnO₂ is its deposition onto a conductive substrate. This well-studied method has produced very good results, increasing the gravimetric capacitance to >400 F g⁻¹ [47]. Actually, when the deposited film reaches the-tens-of-nanometer scale, the capacitances next to the theoretical value have been measured (~1250 F g⁻¹) [24]. Still, the areal mass loading is significantly low, which leads to a deficient areal energy density. In addition, the manufacturing costs of the substrate as well as the thin layer deposition technique make this approach difficult to execute for practical applications [24]. Therefore, even if thin layer deposition and other approaches such as doping may be useful ways to deal with the low conductivity, the rational addition of highly conductive carbonaceous materials is a more affordable way to obtain easily scalable electrodes reaching ~400 F g⁻¹ [24,28,48,49].

Since the properties of the electrode materials are crucial for the performance of the SCs, not only the material choice, but also the cell design is critical for an optimal operation. In this regard, much attention has been devoted to hybrid systems that operate with an EDLC electrode and a pseudocapacitive or battery-type electrode. These hybrid systems are designed in order to benefit from the advantages of each type of electrode, counteracting their individual weaknesses. Hybrid systems can also make use of the different potential windows of the electrodes, and thus increase the operation voltage of the cell, enhancing the overall energy density [50].

In the present report, an aqueous hybrid SC system is proposed, which works with an EDCL-type negative electrode made of an AC and a PC-type MnO₂/carbon black composite positive electrode. MnO₂ was synthesized in two different polymorphs, the previously mentioned α-MnO₂ and δ-MnO₂ phases, while the AC was commercial. The MnO₂ and AC electrodes were characterized in three different aqueous electrolytes in order to choose the best combination to build a full hybrid cell. The three chosen aqueous electrolytes were 1 M KOH, 0.5 M Na₂SO₄ and 0.5 M Na₂SO₄ + 0.2 mM MnSO₄. This work aims to compete with the more common metal–ion hybrids, while benefiting from the stability, safety, and low material and manufacturing cost of aqueous systems. The nanostructured MnO₂ used as an electrode-active material, obtained by a one-step hydrothermal synthesis, offers an effective, more affordable alternative to the current state-of-the-art pseudocapacitive materials in the literature. Taken together with the choice of the electrolytes explored here, the proposed system aims to be as sustainable, safe and economical as possible.

2. Materials and Methods

2.1. Synthesis and Physical-Chemical Characterization of MnO₂ Samples

KMnO₄ (0.022 mol, Probus) was reduced with ethylene glycol (0.009 mol, Panreac) in distilled water (200 mL) at room temperature following the synthesis route proposed by Ragupathy et al. The mixture was stirred for 20 min and then MnO₂ was vacuum filtered as a brown solid. After that, it was kept in a furnace at 60 °C until the next day, when the product was ground until it was a powder [51]. The obtained product was heat treated at different temperatures, i.e., 100, 200, 300, 400, 500 and 600 °C in a furnace.

Phase identification of the samples was carried out by X-ray diffraction, XRD (Panalytical X’Pert PRO) between 5 and 70° (2$\mathsf{\theta }$). Raman spectra were obtained using a Renishaw InVia spectrometer (785 nm wavelength, <1.5 mW power). The compositional characterization of the samples was carried out by thermogravimetric analysis, TGA (Ar, 5 °C/min until 800 °C, Netzsch STA 449) and inductively coupled plasma-atomic emission spectroscopy, ICP-AES (Agilent Technologies 5100, Agilent Technologies, Santa Clara, CA, USA). The morphology of the samples was studied by scanning electron microscopy, SEM (JEOL JSM-7000F, JEOL Ltd., Tokyo, Japan). The homogeneity of the samples was observed by energy-dispersive X-ray spectroscopy, EDX, mapping analysis (Carl Zeiss EVO-40 with Oxford Instruments X-Max, Carl Zeiss, Baden-Württemberg, Germany). The SSA values were estimated by applying the Brunauer–Emmett–Teller theory, BET, to the isotherms obtained from nitrogen adsorption/desorption measurements (0 and 273 K, Quantachrome AutosorbIQ, Anton Paar GmbH, Graz, Austria). Previous degasification was performed at 80 °C for 3 h and under 10⁻⁴ bar vacuum.

2.2. Preparation of Electrodes

Positive electrode composition was 70 wt% MnO₂, 20 wt% conductive carbon black (Timcal Super 65) and 10 wt% polytetrafluoroethylene, PTFE (60 wt% dispersion in H₂O, Sigma-Aldrich, St. Louis, MO, USA). Negative electrode composition was 90 wt% commercial activated carbon (SSA 1600 m² g⁻¹, NORIT DLC Super 30, Sigma-Aldrich, St. Louis, MO, USA) and 10 wt% PTFE. The purpose of adding carbon black to the active material was to enhance its conductivity to achieve a better electrochemical performance, while PTFE was the binder, which brings plasticity to the composite material. The mixtures were drenched in EtOH and blended until gaining enough plasticity to make a black film (~150 μm thickness). After letting the film dry in a vacuum oven at 80 °C for 12 h, it was cut into 11 mm diameter circles, which were weighted and labelled to be used as electrodes afterwards.

2.3. Electrochemical Characterization

Before the electrochemical characterization of the hybrid system, both positive (MnO₂) and negative (AC) electrodes were tested in Swagelok^®-type 3-electrode cells (Swagelok^®, Solon, OH, USA) using an oversized AC counter electrode and a Ag/AgCl (3 M KCl, Metrohm, Herisau, Switzerland) reference electrode. Glass microfiber (GF/A, Whatman, Maidstone, UK) served as a separator. The systems were tested using cyclic voltammetry, CV (BioLogic VMP3, BioLogic, Orlando, FL, USA) at 5, 10, 20, 50, 100 and 200 mV s⁻¹ sweep rates. Three aqueous electrolytes were tested, 0.5 M Na₂SO₄ (referred to in this work as just Na₂SO₄), 1 M KOH (hereinafter referred to as KOH) and 0.5 M Na₂SO₄ + 0.2 mM MnSO₄ (hereinafter referred to as Na₂SO₄ + MnSO₄). The latter electrolyte was chosen because the addition of 0.2–1 mM Mn²⁺ into Na₂SO₄ electrolyte had proven to improve the electrochemical response of MnO₂ electrodes by avoiding the Mn²⁺ dissolution [52]. Final hybrid systems were tested in Swagelok^®-type 2-electrode cells (Swagelok^®, Solon, OH, USA) by CV at 5, 10, 20, 50, 100 and 200 mV s⁻¹ and galvanostatic charge/discharges, GA, at 0.1, 0.5, 1, 2, 5, 7, 10 and 15 A g⁻¹ current densities, calculated in terms of the mass of both electrodes. Finally, with the purpose of investigating the cyclic stability of the proposed system, 5000 GA cycles were carried out at a current density of 1 A g⁻¹.

3. Results and Discussion

3.1. Structural Characterization of MnO₂ Composite Electrodes

The XRD pattern of the MnO₂ sample as synthesized and those obtained for the samples thermally treated at different temperatures are presented in Figure 1a. The samples obtained after the different heat treatments exhibit narrower and more intense maxima because of the increased crystallinity and particle size. The profile of the diffraction pattern of the MnO₂ sample as synthesized (pristine) has been fitted according to the structure of the δ-MnO₂ (birnessite, JCPDS 43-1456), despite the low intensity and large peak width in Figure 1b. No major changes can be observed until 400 °C. As the heat treatment temperature increases, more diffraction peaks are observable. From 400 °C, the phase transition from δ- to α-MnO₂ is already clearly observable. Upon reaching 600 °C, the consolidation of the phase transition is already clearly distinguishable, making it possible to fit the diffraction pattern with a single phase corresponding to α-MnO₂ (JCPDS 44-0141), as shown in Figure 1c. Thus, δ-MnO₂, the untreated sample (denoted as MnO₂-pr, pristine) and α-MnO₂, the sample obtained at 600 °C (MnO₂-600), which shows the highest crystallinity amongst the treated samples, were selected to establish the effect of the different crystal structures of MnO₂ on the electrochemical response of the material. The δ-MnO₂ structure is composed of layers with tetragonal holes, stabilized by water molecules stored between the sheets, while the α-MnO₂ structure consists of tunnels of 2 × 2 tetragonal holes as shown in Figure 1b,c. These structural differences might affect the electrochemical performance of the compound, as will be discussed later. Samples treated at lower temperatures were not selected as they could more easily have mixed phases of the two different MnO₂ polymorphs.

The structural analysis of the prepared samples was completed by means of Raman spectroscopy. As Figure 2 shows, both samples register two bands at 568 cm⁻¹ and 639 cm⁻¹, which correspond to the stretching and bending modes of [MnO₆] octahedra that MnO₂ oxides commonly show [53,54]. Spectra of MnO₂-600 also show translational shifts of [MnO₆] octahedra on an additional band at 181 cm⁻¹. Modes above 100 cm⁻¹ such as the one previously mentioned are due to long range motions of linked [MnO₆] octahedra that form the 2 × 2 tunnels of cryptomelane. The bands observed in the Raman spectra for both samples are consistent with the structures determined by XRD and are in good agreement with those reported in the literature [53,54,55,56].

3.2. Morphology and Specific Surface Area

The microstructure, particle size and morphology of both MnO₂-pr and MnO₂-600 samples were investigated by SEM. As shown in the SEM images in Figure 3, both samples are composed of agglomerates of particles with sizes below 1 μm. The EDX analysis helped to ensure that the elemental composition of the powder samples are homogeneous, as can be seen in Figure 3c,d,g,h.

Due to the smaller particle size of the MnO₂-pr sample, a much larger SSA could be expected, which would translate into a higher capacitance value, since the redox reactions responsible for the capacitive response take place on the surface. According to IUPAC, the nitrogen adsorption/desorption isotherm of sample MnO₂-pr shown in Figure 4a corresponds to a type IV. It can be related to the formation of a monolayer in the low-pressure zone, followed by a weak bonded multilayer, and the hysteresis curve around 0.7 P/P° could indicate the existence of a mesoporous structure. On the other hand, the isotherm of MnO₂-600 is of type III, which is often related to the formation of random multilayers from the beginning [57]. The calculated BET SSA values are 197 m² g⁻¹ for MnO₂-pr and 24 m² g⁻¹ for MnO₂-600, which uphold the deduction of MnO₂-pr having smaller particle size and larger SSA than the treated sample. As can be observed in the inset of Figure 4a, the non-local density functional theory (NLDFT) treatment was applied to the isotherm registered by the most porous sample, MnO₂-pr, in order to obtain a pores size distribution of the sample. The curve indicates a microporosity with pores, formed by the space between particles, of around 1 nm but also a mesoporosity of wider pores between 5 and 15 nm, averaging at 10 nm.

3.3. Compositional Characterization of MnO₂: Thermogravimetric Analysis and Inductively Coupled Plasma-Atomic Emission Spectroscopy

Figure 4b shows the TGA curves for both MnO₂-pr and MnO₂-600 samples performed under Ar atmosphere and up to 800 °C. The mass losses between 100 and 200 °C would correspond to the H₂O molecules adsorbed on the surface of the materials, 10.5% for sample MnO₂-pr and 2.8% for MnO₂-600. Subsequently, between 200 and 600 °C, a mass loss of 2–4% has been measured in MnO₂-pr. This fact may be due to the loss of water molecules stored between layers in the layered structure of the thermally untreated sample. During the heat treatment, a reorganization of the oxide structure takes place due to the destabilization of the layered structure, moving from δ-MnO₂ to α-MnO₂ [58,59]. On the other hand, in the MnO₂-600 sample, since these internal water molecules have already been lost in the heat treatment, the 2.5% mass loss in that temperature range may be due to the release of adsorbed CO₂ molecules [60]. Finally, between 600 and 800 °C, a third mass loss occurs, probably corresponding to the release of oxygen due to the partial reduction of Mn(IV) [59].

Since the synthesis of the MnO₂ samples is based on the reduction of potassium permanganate, IPC-AES measurements were performed to determine the amount of potassium in the samples. The calculated atomic ratios of K:Mn are 0.27:1(MnO₂-pr) and 0.26:1 (MnO₂-600). Therefore, potassium is present in both samples despite the thermal treatment. These data, together with TGA results, made it possible to obtain the exact formulas of the two samples: K_0.27MnO₂·0.27H₂O in the untreated sample, and K_0.26MnO₂, when treated at 600 °C. As Qu et al., explained, MnO₂ samples with this K:Mn ratio contain K⁺ ions and water molecules as pillars to help with stabilizing the crystalline structure between the sheets. Furthermore, the authors obtained similar XRD diffraction patterns before and after 10,000 charge/discharge cycles, concluding that there are almost no changes in the crystalline structure during the long-term cycling [61].

3.4. Electrochemical Characterization of MnO₂ Electrodes

Before building the hybrid systems, the electrochemical study of each material was performed. Figure 5 shows the CV curves of the MnO₂-pr and MnO₂-600 samples along with the measurements of the commercial AC. The CV curves of the AC exhibit a rectangular-like shape in all three electrolytes, i.e., Na₂SO₄, KOH and Na₂SO₄ + MnSO₄, typical of capacitive behaviour. Oxide samples, however, show more irregular profiles due to the Faradaic charge transfer reactions [62].

Furthermore, the manganese dioxide samples display potential windows at more positive values than the AC electrodes, confirming that they are more suitable as positive electrodes. The MnO₂-pr sample reaches much higher capacitance values than the thermal treated sample in all three electrolytes, although the MnO₂-600 sample is stable in a wider potential window (+0.2 V). Figure 6 compiles the capacitance values obtained at the different sweep rates for all three samples in all three electrolytes.

In all three cases, capacitance values in the Na₂SO₄ + MnSO₄ electrolyte are slightly higher than in Na₂SO₄; thus, the presence of Mn²⁺ species may have a positive effect on the electrochemical response [52]. Therefore, it has been thought to exclude the Na₂SO₄ electrolyte for the final system. The results obtained in the KOH electrolyte show greater differences. The working potential windows are shifted towards more negative potential values, and narrower windows than in sulphated electrolytes (0.8 V vs. 1.2 V) are observed, as can be observed in Figure 5. This behaviour fits with the general tendency of neutral electrolytes to present wider potential windows than alkaline ones [63]. The narrower potential window is a disadvantage, since the potential range contributes positively to the energy stored by the system. However, the MnO₂-pr sample exhibits a higher capacitance value in the KOH electrolyte compared to the values obtained in the sulphated electrolytes (237 F g⁻¹ vs. 180 F g⁻¹). Thus, to conclude which electrolyte will have a more positive impact on the electrochemical response of the final system, a MnO₂-pr//AC final system is set up in both Na₂SO₄ + MnSO₄ and KOH electrolytes.

To optimize the system and to balance the negative and positive charges through the appropriate mass balance, it is necessary to know the capacity of the individual electrodes, as the capacity per mass unit represents the accumulated or released charge in the electrode. Figure 6 also shows this parameter with respect to the discharge time. In the Na₂SO₄ + MnSO₄ electrolyte, the MnO₂-pr electrode, except at very short discharge times, generally presents twice the capacity of the AC; therefore, the best mass balance for the final system would be 1:2, MnO₂-pr:AC. In the KOH electrolyte, on the other hand, the two electrodes show equal capacitance values over the entire discharge times studied, so a 1:1 mass balance is used in that case.

3.5. Electrochemical Characterization of the Final Systems

The working potential window of the final system in each of the electrolytes was estimated by voltammetry. As Figure 7 reports, both in alkali and neutral electrolytes the MnO₂-pr//AC system exhibits CVs with a square profile in all of the explored sweep rates. The GAs were performed to calculate specific capacitances in the selected potential ranges and the charge/discharge profiles are linear at all current densities used (see Figure 7). The cells working in the Na₂SO₄ + MnSO₄ electrolyte are able to operate at a 2 V cell voltage while those using KOH work at a cell voltage of 1.5 V. Specific capacitances were calculated from the GA cycles and are displayed in Figure 7. Excepting at current densities below 0.5 A g⁻¹, the sulphated electrolyte obtains higher capacitances than KOH.

To examine in depth the behaviour of each electrode in the system, the CV curve of each electrode is presented in Figure 8. In the Na₂SO₄ + MnSO₄ electrolyte, the operating potential range of the negative electrode is −0.7–0.2 V vs. Ag/AgCl and the positive is 0.2–1.4 V vs. Ag/AgCl, which are slightly lower than those in Figure 5. This suggests that these potential windows could be expanded by slightly changing the mass balance. Furthermore, it can be observed that the positive electrode achieves higher specific capacitance values due to the different mass loadings on the electrodes. In the KOH electrolyte, the negative AC electrode works between −1.1 and −0.25 V vs. Ag/AgCl and the positive between −0.25 and 0.4 V vs. Ag/AgCl, obtaining similar current values. Once again, both potential windows have been slightly lower than those measured in the 3-electrode cells (Figure 5); therefore, it might be possible to extend the cell voltage to enhance the energy storage.

As can be seen in Figure 9, the system built with the Na₂SO₄ + MnSO₄ electrolyte has shown higher capacitances in all of the current densities above 0.5 A g⁻¹, and it has been stable in wider operating voltage values, as shown in Figure 8. These results lead to expected higher energy density values in that system. In Figure 10a, a “Ragone plot” has been charted, which compares energy density against power density.

Na₂SO₄ + MnSO₄ has reported higher energy densities for all of the measured specific powers, so it can be concluded that it is a most suitable electrolyte for this system. Furthermore, the neutral nature of Na₂SO₄ + MnSO₄ plays in favour of the sustainability and the useful life of the cell, since non-neutral aqueous electrolytes usually present technical drawbacks, mainly due their corrosive character [63]. To find out how the system behaves over time, it was cycled with 1 A g⁻¹ for 5000 GA charge/discharge cycles, as shown in Figure 10b. During the cyclability study, both electrodes remain stable, far exceeding 80% capacitance retention. In the first cycles (<1000 charge/discharge cycles), known as the pre-adaptation cycles, both show an increase in capacitance of approximately 15% because the system did not undergo the pre-conditioning cycles, as might be expected from commercial cells. Still, given the high retention obtained in these measurements, i.e., almost no change after 5000 cycles, both systems could be considered as potential candidates for high-cyclability aqueous hybrid electrochemical capacitors [64]. The latest literature reporting MnO₂-based asymmetric systems rely on complex composite materials, ultrathin layers and N-doped carbonaceous materials [64,65,66,67,68]. The present work manages to achieve similar results, in the same order of magnitude and in a simpler and more scalable way, which supports the fact that the simpler manufacturing process of aqueous pseudocapacitive asymmetric systems is an additional asset of these energy storage devices.

The use of MnO₂ as a pseudocapacitive material continues to be the focus of attention in research. The advances in the green synthesis and in the electrochemical performance of this material are pushing it towards an increasingly near-possible commercialization. The road ahead possibly awaits many challenges, but it is worthwhile to take advantage of the excellent properties of this material in a progressively cheaper, sustainable and simpler way. In addition, the advances made in this aspect could not only be used in energy storage systems but also in other areas of knowledge.

4. Conclusions

In summary, in this study, laboratory-grade hybrid supercapacitor cells have been successfully constructed using δ-MnO₂ as the positive electrodes and a commercial activated carbon as the negative electrode. The nanostructured δ-MnO₂ with the formula K_0.27MnO₂·0.27 H₂O was prepared by reducing KMnO₄ with ethylene glycol. Later, a 600 °C heat treatment was applied to the sample, changing the crystalline structure and particle size of the initial compound from the δ-MnO₂ layered phase to a α-MnO₂ 2 × 2 tunnel phase with the K_0.26MnO₂ formula. These samples present the highest capacitance values in the 1 M KOH electrolyte, but they can work in a wider potential window in the 0.5 M Na₂SO₄ + 0.2 mM MnSO₄ electrolyte; thus, two final systems have been built, one with each electrolyte. Due to the wider voltage obtained in the sulphated electrolyte (2.0 V vs. 1.5 V) and the higher capacitance values obtained in general, it has been concluded that the 0.5 M Na₂SO₄ + 0.2 mM MnSO₄ electrolyte is more suitable for this δ-MnO₂//AC combination. The system has shown an energy density of 15.6 Wh kg⁻¹ at a power of 1.0 kW kg⁻¹ and no capacitance loss after 5000 charge/discharge cycles.