Jun
Ni
a,
Weijian
Chen
a,
Xinyang
Zhang
a,
Hui
Xu
a,
Minghui
Zhang
*b and
Xiaoliang
Wu
*a
aCollege of Chemistry, Chemical Engineering and Resource Utilization, Northeast Forestry University, 26 Hexing Road, Harbin 150040, P. R. China. E-mail: wuxiaoliang90@163.com
bSchool of Pharmacy, Health Science Center, Xi'an Jiaotong University, Xi'an, Shaanxi 710049, PR China. E-mail: minghuizhang@xjtu.edu.cn
First published on 20th June 2025
Heteroatom-doped hierarchical porous carbon materials demonstrate significant promise for energy storage applications. In this paper, nitrogen-doped hierarchical porous carbon (NPC) materials were synthesized by one-step carbonization process using agar as the carbon precursor, urea as the nitrogen precursor, and KHCO3 as the activating agent. Owing to the combined influence of substantial nitrogen and oxygen functional groups, interconnected hierarchical porous structure and large specific surface area, the NPC-600 electrode delivers a high specific capacitance of 450 F g−1 and remarkable cyclic stability. Moreover, the NPC-600//NPC-600 symmetrical supercapacitor delivers an energy density of 29.41 Wh kg−1 and good cyclic performance. More interestingly, a zinc ion hybrid capacitor (ZIHC) constructed with NPC-600 as the positive electrode achieves a capacitance of 368.78 F g−1 (163.9 mAh g−1), an energy density reaching 120.75 Wh kg−1 and superior cyclic characteristics. The research affords a straightforward way for fabricating heteroatom-doped porous carbon as electrode for supercapacitor and ZIHCs.
Keywords: Hierarchical porous carbon; KHCO3; Agar; Supercapacitor; Zinc ion hybrid capacitor.
Zinc ion hybrid capacitors (ZIHCs) can adeptly combine the advantages of supercapacitors (outstanding electrochemical stability and superior power density) and zinc ion batteries (excellent energy density), which has attracted extensive attention in recent years.9–11 Zinc foil anodes are considered as promising negative electrodes because of the great abundance of zinc metal on the earth (300 times larger than lithium), high theoretical volumetric capacity and gravimetric capacity (5851 mAh cm−3 and 820 mAh g−1), appropriate potential (−0.76 V vs. standard hydrogen electrodes) and excellent stability in both air and H2O.12,13 Porous carbon materials show great potential as cathode materials for ZIHCs attributed to the affordable price, adjustable pore structure, elevated specific surface area and outstanding electrochemical robustness.14,15 Due to the limitation of the electronic double-layer energy storage mechanism, the energy density of porous carbon-based ZIHCs still cannot satisfy the requirements for high energy density EES.16
Enhancing the electrochemical capabilities of porous carbon materials can be significantly achieved by designing hierarchical porous structure and regulating the pore structure.17–19 Generally, micropores contribute to the physical adsorption of ions at the electrolyte/electrode interface, thus contributing to the energy storage.20–22 Mesopores may provide high-speed channels for fast passage of ions, while macropores can serve as ion buffer pools and provide enough space for ion accommodation.23 Furthermore, introducing heteroatom functional groups into carbon materials can promote the chemical adsorption of Zn2+ by introducing more electrochemical active sites, thus improving the charge storage capacity of positive carbon electrodes.24,25 In particular, the nitrogen doping strategy can elevate the chemisorption of zinc ions on their surface, effectively enhancing the energy density of ZIHCs.3
Herein, we developed a single-step carbonization process to synthesize nitrogen-enriched hierarchical porous carbon (NPC) by utilizing agar as a carbon source, urea as a nitrogen source and KHCO3 as an activator. Thanks to the combined influence of the significant nitrogen and oxygen functional group content, three-dimensional (3D) interconnected hierarchical porous structure and expansive specific surface area, the NPC-600 electrode delivers a specific capacitance of 450 F g−1 and superior cycle performance. Furthermore, the assembled NPC-600//NPC-600 symmetrical supercapacitor achieves an energy density of 29.41 Wh kg−1 and excellent cycle performance. Moreover, the ZIHC using NPC-600 as a cathode delivers a high capacitance of 368.78 F g−1 (163.9 mAh g−1), an impressive energy density of 120.75 Wh kg−1 (100 W kg−1), and exceptional cycle stability.
2KHCO3 → K2CO3 + CO2 + H2O | (1) |
K2CO3 + C → K2O + 2CO | (2) |
K2CO3 → K2O + CO2 | (3) |
K2O + C → 2K + CO | (4) |
CO2 + C → 2CO | (5) |
CO(NH2)2 → NH3 + HCNO | (6) |
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Fig. 2 (a and b) SEM images of NPC-600; (c) TEM image of NPC-600; (d) high resolution TEM image of NPC-600; (e) elemental mapping images of NPC-600: C (f), N (g) and O (h). |
An X-ray diffractometer (XRD) was employed to test the crystallographic structure of the specimens. As illustrated in Fig. 3a, all samples exhibit two broad and faint peaks at around 24.6° and 43.1°, corresponding to the (002) and (100) crystal planes of carbon materials. These two broad and faint peaks confirm that there are massive disordered porous structures in carbon samples. In addition, with the rise in temperature, the peak's intensity diminishes, attributed to the elevated temperatures favoring the activation and formation of a more disordered porous structure. The disordered porous structure was further evaluated by Raman. As shown in Fig. 3b, the ID/IG values of NPC-500, NPC-600 and NPC-700 are 0.9394, 0.9647 and 0.9920, respectively, which indicates that as the temperature increases, more disordered porous structures are generated, aligning closely with the XRD findings.30–32 Furthermore, the moderate ID/IG value also indicates that NPC-600 has suitable disordered structures.
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Fig. 3 (a) XRD patterns of NPC-500, NPC-600 and NPC-700; (b) Raman spectra of NPC-500, NPC-600 and NPC-700. |
The material constituents and surface elements of the NPCs were examined via X-ray photoelectron spectroscopy (XPS). Fig. 4a displays three distinct peaks at 284.7 eV, 400.1 eV, and 531.9 eV, corresponding to C 1s, N 1s, and O 1s, respectively. The elemental analysis of NPC-600 indicates that the proportions of N and O are 5.30 at% and 10.65 at%. As illustrated in Fig. 4b, the C 1s spectrum with high resolution reveals four distinct peaks at 283.74 eV, 284.8 eV, 285.71 eV, and 287.05 eV, assigned to C–C, C–N, C–O, and CO linkages, respectively. Fig. 4c presents the high-resolution N 1s spectrum with four peaks, which are attributed to pyridine N at 398.08 eV, pyrrole N at 399.48 eV, graphite N at 400.88 eV, and pyridine N oxide at 402.73 eV. Among these, N-6 and N-5 can produce pseudo-capacitance via the Faraday reaction, and N-Q adds two electrons to the conductive π system, increasing the prepared sample's conductivity.33,34 As illustrated in Fig. 4d, the binding energies of the three peaks in the O 1s spectrum: C
O, C–O and O
C–O are 530.27 eV, 531.41 eV and 532.43 eV, respectively. The trends of the elemental composition values of carbon, nitrogen and oxygen in each NPC sample varying with temperature are shown in Table S1.† It can be seen from the table that the content of carbon atoms increases gradually with the increase of temperature, while the content of nitrogen atoms and oxygen atoms decreases gradually with the increase of temperature. From the percentage change trend of each element with temperature shown in Table S2,† it can be seen that the proportions of N-6 and N-5 in NPC-600 are 66.27% and 22.90%, respectively, which are higher than those in the other two samples. N-6 and N-5 are the main contributors to providing pseudo-capacitance, indicating that the introduction of N atoms has a remarkable effect. The presence of heteroatoms in the carbon material surface can not only significantly improve their wettability, but also participate in the redox reaction (Fig. S2†), providing additional pseudo-capacitance.
Nitrogen adsorption–desorption isotherm was employed to analyze the porosity of the carbon specimens. As illustrated in Fig. 4e, the three isotherms are similar in shape, aligning with the characteristic type I and type IV binding curves. In addition, under low relative pressure (P/P0 < 0.01), sudden increase in pressure and high relative pressure (P/P0 > 0.45) present a distinct hysteresis loop, which proves that micropores and mesopores/macropores exist in the samples. Table 1 illustrates the detailed surface area and pore structure parameters of the NPC specimens. As the temperature increases, the specific surface area of the NPC specimens enhances from 631.76 m2 g−1 (NPC-500), climbing up to 1056.2 m2 g−1 (NPC-600), and reaching 1890.1 m2 g−1 (NPC-700). Through the application of density functional theory (DFT), the material's pore size distribution was determined. The NPC-600 sample displayed pore sizes falling within 0.8 nm to 1.1 nm, contributing favorably to energy storage (Fig. 4f).29,31
Samples | S BET (m2 g−1) | S mic (m2 g−1) | S me (m2 g−1) | S me/Smic | V total (cm3 g−1) | D (nm) |
---|---|---|---|---|---|---|
a Specific surface area (SBET) was calculated with a modified Brunauer–Emmett–Teller (BET) method. b Micropore surface area (Smic) was obtained from the t-plot method. c Mesopore surface area (Sme) was obtained from the t-plot method. d Total pore volume (Vtotal) was estimated from the adsorbed amount at a relative pressure of 0.99. e Average pore diameter (D) was obtained from D = 4Vtotal/SBET. | ||||||
NPC-500 | 631.8 | 532.28 | 99.48 | 0.19 | 0.30 | 1.93 |
NPC-600 | 1056.2 | 901.36 | 154.84 | 0.17 | 0.49 | 1.86 |
NPC-700 | 1890.1 | 1471.30 | 418.80 | 0.29 | 0.93 | 1.96 |
Cyclic voltammetry (CV), galvanostatic charge–discharge (GCD), as well as electrochemical impedance spectroscopy (EIS) analyses, were conducted in a 6 M KOH aqueous solution utilizing a three-electrode configuration to assess the electrochemical capabilities. As depicted in Fig. 5a, CV curves of the three electrodes at 50 mV s−1 are quasi-rectangular shapes with faradaic humps, meaning that partial capacity comes from the contribution of Faraday pseudo-capacitance. Moreover, the NPC-600 electrode exhibits the biggest integration area, corresponding to the highest specific capacitance. As illustrated in Fig. S3,† consistent with the CV results, the NPC-600 electrode displays the longest discharge time, implying superior specific capacitance. As illustrated in Fig. 5b, when the scanning rate increases to 100 mV s−1, the CV curve of the NPC-600 electrode still keeps a quasi-rectangular shape, demonstrating superior rate characteristic. According to the discharge time (Fig. 5c), the NPC-600 electrode achieves a specific capacitance of 450 F g−1 at 0.5 A g−1, outperforming NPC-500 (326 F g−1) and NPC-700 (428 F g−1) and other reported porous carbon in the literature (Fig. 5d). At the same time, as illustrated in Fig. 5e, after 10000 cycles at 200 mV s−1, NPC-600 shows a capacitance retention rate of 91.31% (244.57 F g−1), suggesting superior cyclic stability. The Nyquist diagrams of the NPC-600 electrode shows a small semicircle alongside a steep line, exhibiting a phase angle near 90° within the low frequency zone. Moreover, in the high frequency zone, the semicircle's center and the center shift away from the real axis (Fig. 5f). In the equivalent circuit, the value of solution resistance (Rs) is ascertained by the point where the curve meets the real axis at the upper frequency limit, which represents the equivalent series internal resistance related to electrode materials, contacts and electrolytes, and the value of charge transfer resistance (Rct) is identified by the radius of the distorted semicircle observed in the high frequency domain, denoting the resistance to charge transfer pertinent to the Faraday redox reaction. The Rs and Rct of NPC-600 are 0.55 Ω and 0.16 Ω, respectively, indicating good conductivity and a fast ion diffusion rate. In addition, we also tested the hydrogen evolution reaction (HER) electrocatalytic activity in a three-electrode system. The linear sweep voltammetry (LSV) map showed that NPC-600 showed good HER activity (Fig. S4a†). The linear fitting of the Tafel curve is carried out by the following Tafel equation (Fig. S4b†), and the Tafel slope of NPC-600 is 389 mV per decade, which further illustrates the good HER dynamics.
The NPC-600//NPC-600 symmetrical supercapacitor was constructed in 2 M ZnSO4 aqueous solution. The CV analysis was performed at 50 mV s−1 to determine the optimized voltage testing range. The CV curve of the NPC-600//NPC-600 symmetrical supercapacitor maintained its integrity even at the voltage range of 0–1.8 V, showing no obvious deformation (Fig. 6a). Thus, the working voltage range is determined as the voltage range from 0 up to 1.8 V. As depicted in Fig. 6b, the CV measurements for the NPC-600//NPC-600 symmetrical supercapacitor span from 2 mV s−1 to 100 mV s−1. Along with the scanning rate increasing, the CV curve shows no obvious deformation, indicating excellent rate behavior. Fig. 6c depicts the GCD plots for the NPC-600//NPC-600 symmetric supercapacitor under diverse current densities. By evaluating the discharge durations, the specific capacitance for the symmetric supercapacitor was estimated. As illustrated in Fig. 6d, the NPC-600//NPC-600 symmetric supercapacitor achieves a specific capacitance of 65.37 F g−1 at a current density of 0.25 A g−1. As illustrated in Fig. 6e, the NPC-600//NPC-600 symmetrical supercapacitor boasts an impressive energy density of 29.41 Wh kg−1 (300 W kg−1) thanks to its extensive voltage window and elevated specific capacitance, which is higher than those reported in other documents.12,35–40 As illustrated in Fig. 6f, the capacitance retention rate of the NPC-600//NPC-600 symmetrical supercapacitor is 92.05% after 10000 cycles at a scanning rate of 200 mV s−1, reflecting its excellent electrochemical performance.
A zinc ion hybrid capacitor utilizing NPC-600 as the cathode and zinc foil as the anode in 2 M ZnSO4 solution was constructed to assess the electrochemical characteristics of the electrode materials in practical applications. As illustrated in Fig. 7a, the CV graphs exhibit a rectangular shape, and the redox peak is reversible, confirming that the ZIHC operates via a mechanism that encompasses both battery and supercapacitor characteristics.41–46 Even at 100 mV s−1, the rectangular shape will not change significantly, reflecting excellent rate behavior. As illustrated in Fig. 7b, the GCD plots for the Zn//ZnSO4//NPC-600 hybrid capacitor maintain their form as the current density escalates, demonstrating consistent reversibility. However, in the Nyquist diagram of ZIHC (Fig. S5†), a prominently deformed semicircle and a distinct line with a gradient below 1 in the high frequency range are observed, signifying a high Rct value and a notable ion diffusion resistance. This is not only related to the poor diffusion of hydrated Zn2+ and the planar structure on the surface of the zinc foil electrode, but also related to the inefficient Zn2+ plating/stripping processes and kinetics.47,48
Fig. 7c shows a comparison chart of ZIHC capacitance attenuation. It has been computed that the peak specific capacitance for ZIHC utilizing NPC-600 as the cathode material can hit 368.78 F g−1 (163.9 mAh g−1) when subjected to 0.1 A g−1. Concurrently, for ZIHC systems with NPC-500 and NPC-700 cathodes, their respective maximum specific capacitance values are 276.75 F g−1 (123 mAh g−1) and 360.9 F g−1 (160.4 mAh g−1). Notably, the Zn//ZnSO4//NPC-600 hybrid capacitor is capable of sustaining a capacitance level of 106.88 F g−1 (47.5 mAh g−1) even at 10 A g−1, highlighting its superior charge–discharge attributes. Fig. 7d illustrates the GCD profiles of the ZIHC based on different NPC cathodes of 0.1 A g−1, and it is found that the specific capacitance of the Zn//ZnSO4//NPC-600 hybrid capacitor is the highest among the three. At the same time, it also validates the hybrid energy storage mechanism that the curve deviates from the standard symmetrical linear shape. In Fig. 7e, the ZIHC with NPC-600 as the cathode can reach an impressive energy density of 120.75 Wh kg−1 (100 W kg−1), surpassing previously documented ZIHC values.12,41,49–56 The cycle stability of the Zn//ZnSO4//NPC-600 hybrid capacitor was tested at 5 A g−1, where it retained 84.25% of its initial value after 10000 cycles (Fig. 7f), showing outstanding cycling performance.
Through the computation of the distinct charge storage processes' contributions to the overall capacitance and examination of the CV curve's electrochemical dynamics, the electrochemical activity of the NPC-600 cathode in a hybrid capacitor was initially grasped. The CV test was carried out over a scanning rate range from 5 mV s−1 to 100 mV s−1, and the non-rectangular CV profile can indicate the mixed charge storage mechanism (Fig. S7†). Upon setting the scanning rate to 5 mV s−1, about 67.97% of NPC-600's total current was governed by diffusion control, as indicated by the purple shaded area. In general, two formulas are applicable for assessing the current response across varying voltages:12
i = avb | (1) |
log(i) = b × log(v) + log(a) | (2) |
In adherence to the mentioned formula, when the value of b hovers around 0.5, it signifies that the electrochemical reaction is predominantly governed by diffusion. Conversely, when b tends towards 1, it suggests that a capacitive reaction is at play. As indicated by the reduction process data, the computed value of b is 0.75 (refer to Fig. 8a), suggesting that the charge storage mechanism in the zinc ion hybrid capacitor, utilizing NPC-600 as the cathode, is primarily dominated by capacitance and diffusion. Notably, the calculated values of b for the other samples are 0.71 and 0.89, respectively (Fig. S6a†), which indicates that the charge storage mechanism in zinc ion hybrid capacitors using them as cathodes is also mainly controlled by capacitance and diffusion. Moreover, the following formula can be used to quantitatively calculate the current response at a given voltage: i = k1v + k2v1/2, where k1v and k2v1/2 respectively represent the capacitance and diffusion control process. Based on the formula, the current response contribution rate is calculated. As illustrated in Fig. 8b, the capacitance contribution ratio exhibits a direct correlation with the scanning rate. At slower scanning rates, diffusion plays a dominant role in the contribution. As the scanning rate rises, the diffusion contribution percentage steadily diminishes, and concurrently, the capacitance behavior contribution percentage, thereby confirming that the NPC-600 cathode in the ZIHC operates with a hybrid control mechanism for energy storage. The data for different scanning rates are illustrated in Fig. S7.† As the scanning rate escalates to 100 mV s−1, the percentage of capacitance contribution also increased to 72.43%, which proves that the NPC-600 electrode has a fast dynamic process and capacitance control behavior at a fast scanning rate. These findings suggest that ions tend to be accommodated near the electrode surface during the reaction, helping to prevent the degradation of the electrode material's structure. Furthermore, the capacitance reaction process efficiently reduces the electrolyte ion transmission route, thereby enhancing the rate capability of the electrode and boosting the overall functionality of electrochemical energy storage systems. The exceptional performance of NPC-600 can be credited to its distinct stratified porosity configuration, as well as the contribution of the N and O functional groups.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5im00044k |
This journal is © Institute of Process Engineering of CAS 2025 |