Introduction

In recent years, energy consumption has increased worldwide as human well-being has become increasingly reliant on digital tools, and consequently, the need for high-performance energy storage systems has become prominent [1, 2]. The application of decentralized energy resources and storage technologies in the field of portable, flexible, and smart electronics has significant challenges that need to be addressed in the global context of energy transition [3, 4]. In this regard, flexible energy devices such as batteries and supercapacitors are key technologies for powering body-worn consumer electronics, sensors, or low-energy bioelectronics (e.g., on-skin diagnostics). Similarly, supercapacitors (SCs) that can fit into various device structures and installation spaces are key enablers for buffering excess energy. SCs have gained increasing attention owing to their fast charge and discharge rates, high power density, long cycle life, and high reliability [5,6,7]. However, endowing conventional SCs with good flexibility as well as high energy density is challenging because both charge collectors (substrates) and electrode materials can experience fracture and delamination during flexing. These supercapacitors can be classified into two types: electrical double-layer capacitors (EDLCs), which usually use carbon active materials, and faradaic capacitors, which use redox-active materials [8]. EDLC devices store electrochemical energy via electrostatic accumulation of charges in the electric double layer and currently dominate the SC market because of their ability to accumulate large amounts of charge [9]. However, their relatively low specific capacitance is inhibitive for the increasing requirements of SCs with higher electrochemical performance, which also restricts their potential large-scale applications [10, 11]. Recently, researchers have focused on exploring faradaic capacitors owing to their high specific capacitance, which is induced by fast reversible redox reactions [12]. Faradaic capacitors generally use a metal oxide/hydroxide as the cathode for efficient redox reaction on the electrode surface, which requires an electrode material with a large specific surface area and good electrochemical activity. Transition metal oxides and hydroxides [13, 14], such as NiO [15], Ni(OH)2 [16], Co3O4 [17], MnO2 [18], and RuO2 [19], and their binary composites have been considered as optimized materials for SCs. The reversible redox reaction in faradaic capacitors occurs on the surface of the electrode, and because the electrical energy is stored on the electrode surface, the storage capacity of faradaic capacitors is significantly influenced by electrode material properties. For this reason, binary NiCu-oxide/hydroxide compounds, which exhibit rich redox reactions due to their multiple oxidation states, have been widely used as faradaic capacitors electrodes. For example, Zhenyuan et al. fabricated NiO/Co3O4 ultrathin nanosheets that have a specific capacitance of 1775 F g−1 at 1 A g−1 [20]. Jun et al. fabricated Cu-metal organic frameworks (MOF) electrodes, which showed a specific capacitance of 318 F g−1 at 1 A g−1 in a KOH electrolyte [21]. Heba et al. prepared Ni–Cu binary phosphides, which exhibited a specific capacitance of 1573 F g−1 at 1 A g [22]. However, oxide and hydroxide composites normally suffer from gradually decreasing stability after several charging and discharging cycles [

Figure 1
figure 1

XRD patterns of the Ni-foam@NiCu(CO3)(OH)2 and PAN@NiCu(CO3)(OH)2 composite electrodes.

Figure 2
figure 2

XPS spectra of the NiCu(CO3)(OH)2 electrode: (a) Ni 2p, (b) Cu 2p, (c) C 1s, and (d) O 1s.

Figure 3
figure 3

SEM images of (a) the Ni-foam, (b) PAN nanofibers as the substrates at similar magnification; Low- and high-magnification SEM images of (c) and (d) the Ni-foam@NiCu(CO3)(OH)2 composite, (e) and (f) the PAN@NiCu(CO3)(OH)2 composite.

Figure 4
figure 4

(a and b) Low-magnification TEM images, (c) HR-TEM image of the PAN@NiCu(CO3)(OH)2 nanowire composite; elemental map** of PAN@NiCu(CO3)(OH)2 nanowires with color coded contribution of Ni, Cu and O (d–f). (g) Elemental contribution according to EDS map** in wt% of PAN@NiCu(CO3)(OH)2 composite.

Electrochemical properties

Figure 5a presents the redox curves of the electrodes with a three-electrode cell, which shows the cyclic voltammetry (CV) curves of the PAN@NiCu(CO3)(OH)2 composite in the potential window of 0.15–0.6 V at scan rates from 5 to 50 mV−1 in a 1 M KOH electrolyte. The oxidation and reduction peaks in the CV curves shifted toward more positive and negative potentials, respectively, as the scan speed increased because the internal diffusion resistance increased within the electrode surface. The typical CV peaks of the PAN@NiCu(CO3)(OH)2 electrodes showed reduction peak at ~ 0.46 V, and an oxidation peak at ~ 0.34 V, respectively, at 10 mV s−1. As the scan rate increased, the redox peak of the PAN@NiCu(CO3)(OH)2 electrode shifted to an extent, indicating that there is the internal resistance of the PAN@NiCu(CO3)(OH)2 electrode. And the CV of PAN@NiCu(CO3)(OH)2 has a large internal area, which is proportional to its capacity value. This result indicates that the PAN@NiCu(CO3)(OH)2 electrode has a great electrochemical value. This electrode exhibits symmetric redox peak property, indicating good performance for redox reactions and largely porous morphology. The CV curves obtained for the PAN@NiCu(CO3)(OH)2 nanowire electrode were standard for faradaic capacitors. The faradaic redox reactions of the NiCu(CO3)(OH)2 composite occurred according to Eqs. (13) [44, 45]:

$${\text{NiCu}}\left( {{\text{CO}}_{{3}} } \right)\left( {{\text{OH}}} \right)_{{2}} + {\text{4OH}}^{-} \rightleftharpoons {\text{NiOOH}} + {\text{CuOOH}} + {\text{CO}}_{3}^{2 - } + {\text{2H}}_{{2}} {\text{O}} + {\text{2e}}^{-},$$
(1)
$${\text{NiOOH}} + {\text{OH}}^{-} \rightleftharpoons {\text{NiO}}_{{2}} + {\text{H}}_{{2}} {\text{O}} + {\text{e}}^{-},$$
(2)
$${\text{CuOOH}} + {\text{OH}}^{-} \rightleftharpoons {\text{CuO}}_{{2}} + {\text{H}}_{{2}} {\text{O}} + {\text{e}}^{-}.$$
(3)
Figure 5
figure 5

(a) The CV curves, (b) galvanostatic CD curves of the PAN@NiCu(CO3)(OH)2 electrode, comparison of (c) the specific capacitance of the NiCu(CO3)(OH)2 composite at different current densities, (d) cycling stability of the NiCu(CO3)(OH)2 on the Ni-foam and PAN substrates.

According to these equations, the redox reactions involve OH from the electrolyte in the optimized NiCu(CO3)(OH)2 composite. Figure 5b shows the galvanostatic charge–discharge (GCD) measurements of the PAN@NiCu(CO3)(OH)2 composite over a potential range of 0–0.45 V. The GCD curves showed a nonlinear slope and triangular symmetry owing to the occurrence of quasi-reversible redox reactions at the electrolyte/electrode interface. As shown in Fig. 5b, the PAN@NiCu(CO3)(OH)2 composite had a long discharge time, indicating that it has high electrochemical performance, which is consistent with the trend observed in the CV analysis. The specific capacities of the previously tested Ni-foam@NiCu(CO3)(OH)2 and PAN@NiCu(CO3)(OH)2 composites were calculated using the following Eq. (4) [46]:

$$Q_{{\text{D}}} = \frac{{I\Delta t}}{m},$$
(4)

where QD (mAh g−1) is the specific capacity, I (mA) is the discharging current, Δt (s) is the discharging time that is measured from 0.0 to 0.45 V, and m (g) is the designated mass of the active material. Using this equation, it was found that the PAN@NiCu(CO3)(OH)2 nanowire composite possessed high electrochemical values. As shown in Fig. 5c, the PAN@NiCu(CO3)(OH)2 electrode exhibited specific capacities of 870, 936, 1025, 960, 899, and 808 mAh g−1, while the specific capacities of the Ni-foam@NiCu(CO3)(OH)2 electrode were calculated to be 759, 632, 496, 424, 364, and 348 mAh g−1 at current densities of 3, 4, 5, 8, 10, and 15 A g−1, respectively. This was attributed to the positive effect of the increased surface area of the PAN@NiCu(CO3)(OH)2 electrode structure. As a result, PAN@NiCu(CO3)(OH)2 had higher specific capacitance values than the NiCu(CO3)(OH)2 composite on the Ni-foam substrate, which indicates the synergetic effect of the PAN nanofibers and NiCu(CO3)(OH)2 nanowire electrode. The cycling properties were also measured to investigate the stability of the electrodes. Long-term electrical retention is an important factor for electrodes in supercapacitor applications and industrialization [47]. As shown in Fig. 5d, after satisfactory cycles, the Ni-foam@NiCu(CO3)(OH)2 and PAN@NiCu(CO3)(OH)2 electrodes exhibited retentions of 88.2% and 84.1%, respectively, after 5000 cycles. The stability of the electrodes was evaluated using the discharging time at a constant current density of 10 A g−1. These results suggest that the Ni-foam@NiCu(CO3)(OH)2 electrode exhibited better cycling stability than the PAN@NiCu(CO3)(OH)2 electrode. The synergistic effects of the PAN substrate and NiCu(CO3)(OH)2 composite contributed to enhanced electrochemical performance for a specific capacitance; however, this electrode possessed a lower retention value owing to its weak polymer properties. Nevertheless, these results indicate better electrochemical properties than those previously reported for NiCu-based electrodes (Table 1). As a result, although the electrode was damaged and the capacity decreased with the increasing number of cycles, it had a high retention value because of the positive influence of the transition metal composites.

TABLE 1 Comparison with the capacitance and retention values of the previously studied nickel- and copper-based electrodes.

To further investigate the viability of the electrodes in energy storage devices, an ASC was fabricated using Ni-foam@NiCu(CO3)(OH)2 and PAN@NiCu(CO3)(OH)2 composites as the cathode and graphene as the anode. A cellulose separator paper and 1 M KOH electrolyte were used for the ASC device. A schematic diagram of the cathode and anode ASC electrodes is shown in Scheme 2. The electrochemical performance of the graphene electrode was measured in the potential range of − 1 to 0 V, as shown in Fig. 6. The CV curves of graphene showed typical rectangular shapes, which represent the ideal faradaic capacitor (Fig. 6a). The GCD curves exhibited linear and symmetric shapes, as shown in Fig. 6b. The specific capacity (Fig. 6c) of the graphene electrode was 122 mAh g−1 at 2 A g−1 and 60 mAh g−1 at 15 A g−1, respectively. EIS analyses were performed to investigate the conductivity behavior and charge-transfer kinetics of the graphene electrode. In the high-frequency region, the graphene electrode showed low Rs and Rct values of 0.6 Ω and 0.82 Ω, respectively (inset of Fig. 6d). The slope of the linear section of the graphene electrode has a higher incline in the low-frequency region, which represents a low Zw value, as shown in Fig. 6d. These results confirmed that the graphene electrode could be a suitable negative electrode for ASCs. Figure 7 shows the CV curves of the assembled ASC, which demonstrate electrical double-layer capacitor properties behavior at different scan rates in the voltage range of 0.0–1.5 V. This phenomenon indicates that PAN@NiCu(CO3)(OH)2 electrode//graphene ASCs were significantly influenced by graphene, which is a negative electrode material. As shown in Fig. 7a, the PAN@NiCu(CO3)(OH)2 composite shows excellent rectangular CV curves, which represent the ideal behavior of SCs. and this ASC device does not have the redox peaks at all scan rates. Figure 7b represents the specific capacity values of the Ni-foam@NiCu(CO3)(OH)2//graphene ASC and PAN@NiCu(CO3)(OH)2 electrode//graphene ASC from the discharge times, which are calculated to be 64 mAh g−1 and 126 mAh g−1 at 2 A g−1, respectively. This improvement in electrical performance is achieved by the electrical conductivity of the active materials and electrolyte penetration provided by the PAN nanofiber substrate to undergo a redox reaction. Therefore, high-speed performance is achieved of the development for high-performance faradaic capacitors. The retention values of the ASCs were measured with respect to the discharge time at a current density of 5 A g−1 in Fig. 7c. The assembled ASC of the Ni-foam@NiCu(CO3)(OH)2 and PAN@NiCu(CO3)(OH)2 electrodes retained 91.3 and 90.1% of their capacities, respectively, after 5000 cycles. The retention values of the ASC were similar after 5000 cycles, regardless of the substrate type. These properties indicate that the PAN@NiCu (CO3)(OH)2 electrode can facilitate a more stable cycle reaction when measuring the electrochemical value with the ASC than with the half-cell electrode. In addition, the energy density and power density were calculated using Eqs. (5) and (6) [64, 65]:

Scheme 2
scheme 2

Configuration of the NiCu(CO3)(OH)2 electrode//graphene ASC device.

Figure 6
figure 6

(a) CV curves of the graphene as electrode in negative voltage window at different scan rates, (b) the galvanostatic CD curves of the graphene at different current densities, (c) the specific capacity of the graphene at different current densities, (d) the EIS spectrum of the graphene as electrode.

Figure 7
figure 7

CV curves of (a) the optimized PAN@NiCu(CO3)(OH)2//graphene ASC; comparison of (b) the specific capacity, (c) cycling stability of the Ni-foam@NiCu(CO3)(OH)2//graphene and PAN@NiCu(CO3)(OH)2//graphene ASCs at 5 A g−1, (d) Ragone plot of the ASC devices.

$$E = \frac{I\int V\mathrm{d}t}{M 3.6},$$
(5)
$$P = E/\Delta t,$$
(6)

where E (Wh kg−1) is the energy density, \(I\)(A) is the applied current, \(\int V\mathrm{d}t\) is the galvanostatic discharge current area, \(M\) (g) is the active mass, P (W kg−1) is the power density, and \(\Delta t\) (s) is the discharge time. Figure 7d presents the ragone plot of the fabricated ASC devices. The PAN@NiCu(CO3)(OH)2 electrode ASC shows that the highest energy density with 90 W h kg−1 at a power density of 835 W kg−1 and current density of 2 A g−1. As the current density changes to 15 A g−1, the energy density decreases to 36 W h kg−1 at a power density of 9268 W kg−1. The PAN@NiCu(CO3)(OH)2 electrode achieved better energy and power densities than that of the Ni-foam@NiCu(CO3)(OH)2 electrode ACS, NiO//carbon [66], Ni(OH)2//carbon [67], and MnO2//carbon [68]. These results can aid the development of flexible and wearable faradaic capacitors with enhanced electrochemical performance by synthesizing PAN nanomeshes and modifying their surface through the growth of binary metal hydroxy-carbonates. Thus, PAN@NiCu(CO3)(OH)2 nanowires are promising materials of the positive electrode for high-performance supercapacitors.