Lingqi
Huang
ab,
Zilong
Gu
a,
Jiayang
Gu
a,
Fei
Zhang
*cf,
Jingshun
Zhuang
a,
Qingzhi
Ma
a,
Tao
Zhang
d,
Jingfei
Li
e,
Heyang
Liu
*ad and
Wei
Feng
*b
aSchool of Environmental and Natural Resources, Zhejiang University of Science and Technology, Hangzhou, 310023, P. R. China. E-mail: heyang.liu@zust.edu.cn
bSchool of Materials Science and Engineering, Tianjin University, Tianjin, 300072, P. R. China. E-mail: weifeng@tju.edu.cn
cLeibniz-Institut für Polymerforschung Dresden e.V. (IPF), Hohe Str. 6, 01069 Dresden, Germany. E-mail: feizhang@tju.edu.cn
dSchool of Biological & Chemical Engineering, Zhejiang University of Science and Technology, Hangzhou, 310023, P. R. China
eZhejiang Institute of Quality Sciences, Hangzhou, 31000, P. R. China
fSchool of Science and Engineering, The Chinese University of Hong Kong, Shenzhen, Shenzhen, Guangdong 518172, P. R. China
First published on 13th July 2024
Conversion of biomass into doped activated carbons (ACs) via green processes is envisioned as a promising path toward modern energy storage applications. ACs are commonly synthesized using strong bases, which are associated with environment and operation risks. Thus, it is necessary to find alternative and green activation reagents. Herein, we report a multi-functional molecular salt (sodium pyrithione) as an activation reagent for the economically viable preparation of doped ACs with a large surface area, rich dopants, and porous structures. The formation of carbons and the variation in the composition and pore architecture were demonstrated. The prepared ACs were then fabricated into cathodes for a zinc-ion capacitor. We correlated the properties of ACs with their performance by analyzing electrochemical measurements. Meanwhile, the optimal SPHC-based ZIC delivered high capacity and excellent cycling stability over 20000 cycles under practical conditions. Moreover, we found that long-term chemical adsorption/desorption on active sites of ACs influences the cathode structure and thus leads to a loss of capacity and changes in the energy storage mechanism. Overall, this work provides an alternative protocol for the synthesis of doped ACs, which can be used as cathodes materials for practical high-performance ZICs.
The traditional route for the synthesis of doped ACs involves high-temperature treatment of pristine carbons with activation reagents and modifiers, but this often requires pristine carbon materials obtained from the pyrolysis of agricultural feed-stocks or certain petroleum-derived products (Scheme 1a).9 Moreover, the treatments commonly involve the use of corrosive activation reagents, organic doping reagents, multiple elevated temperatures, long reaction times, etc.10–12 For example, Ye et al. developed highly porous carbon spheres for battery application, where the carbons were first prepared through catalytic emulsion polymerization using expensive diethynylbenzenes, followed by hydrothermal treatment and activation steps with large amounts of KOH.13,14 Qiu et al. modified the pyrolysis process of lignin by introducing alkali moieties and triazine-based supermolecules in a two-step and slow-heating procedure, which results in the synthesis of high nitrogen-doped carbon for potassium storage application.15 Shen et al. prepared dual-doped ACs using a three-step procedure comprising biochar preparation, KOH activation, and post-treatment with thiourea.16 Regarding practical production conditions, it is highly desirable to avoid the use of hazardous chemicals that exhibit toxicity and pose risk to human health and the environment. Moreover, burdensome processes that require more energy/source input and produce more waste should be avoided when proposing replacement protocols.17 The increasing attention directed toward sustainability from the natural sciences provides incentives to create alternatives to hazardous substances and develop new routes for doped ACs.
Self-activated pyrolysis is an alternative green and sustainable route for the preparation of doped ACs (Scheme 1b). The route can be simple and effective because the carbon texture formation, pore generation, and heterogeneous atom insertion occur within the one-step elevated temperature with the use of specific precursors. For example, Alshareef et al. prepared oxygen-rich ACs by pyrolysis of pyromellitic acid tetrapotassium salt, where the benzene ring, carbonyl group, and potassium work as the carbon source, dopant, and pore generate agent, respectively.2 Similarly, other precursors (such as tetra-alkali metal pyromellitic acid,18 potassium phthalimide,19 and sodium polyacrylate)20 have been recently reported with applicability in the synthesis of advanced doped ACs with the one-step protocol. Similar pyrolysis mechanisms have been demonstrated. Moreover, such protocol eliminates the use of hazardous reagents and reduces burdensome heating processes, allowing for the greener and low energy-demanding production of doped ACs materials. However, such precursors are rare; the prices are higher than common biomass, feed-stocks, or petroleum-derived products; and they often afford limited carbon yields. Engineered co-pyrolysis is another promising route for doped ACs, involving the use of carbonaceous matter and reagents. For example, N/S co-doped porous carbon was synthesized by co-pyrolysis of sodium lignosulfonate and melamine.21 N, O, and F tri-doped porous carbon with a large surface area of carbon (>3000 m2 g−1) was prepared by co-pyrolysis of two powder organic monomers and KOH chips in one batch.22 One advantage of co-pyrolysis is that the post-activation and doping process can be eliminated. Additionally, the required chemicals and materials are versatile, easy to use, cheap, and amenable to large-scale production.
Lignin and hemicellulose are biomass sources mainly composed of carbohydrate units, but exhibit three-dimensional polymer structures and interwoven molecular architectures.23,24 Owing to their attractive structural properties, they have been demonstrated to be appropriate precursors for ACs, and subsequently employed as adsorbers,25 electrode materials,26 anode materials in batteries,27 cathode materials in capacitors,28etc. The utility of lignin and hemicellulose for doped ACs has been extensively investigated due to their merits of being low-cost, renewable, environmentally friendly, and having scale-up potential, etc.5 Nevertheless, traditional treatments and procedures are still the prerequisites. In this work, we sought to develop an alternative green and sustainable route for the preparation of doped ACs via co-pyrolysis of lignin or hemi-lignin in the presence of sodium pyrithione, which is a commercially available cheap ($2–$4 per kg), harmless molecular salt, consisting of N, S, O heteroatoms and Na for self-activation. The proposed process is simple, green, safe, and economical, compared to existing methods (Scheme 1c). Meanwhile, the resultant biomass-derived doped ACs show high surface areas (∼1218 m2 g−1) and are heteroatom-rich. Accordingly, ZICs assembled with biomass-derived doped ACs delivered the highest reversible capacity of 108.6 mA h g−1 and energy density of 67.8 W h kg−1 in aqueous ZIC systems, outperforming traditional ACs that were synthesized with hazardous NaOH. Moreover, the cathodes also displayed excellent cycling stability during the 20000-charge–discharge measurement, indicating its great potential in ZIC application.
Fig. 1a & d shows the SEM images of lignin and hemicellulose-derived carbon materials (LC and HC) without the use of any other regents. The morphologies were inherited from their precursors (Fig. S1†). The pyrolysis allows char yields of 35% and 19% for LC and HC, respectively (Table S1†). Compared to the TGA result, the reduced yield was attributed to one hour of extended pyrolysis at 800 °C. However, the produced carbons show limited surface areas of 2.2 and 6.6 m2 g−1 for LC and HC, respectively. The heterogeneity of the surface area is affected by the composition and pyrolysis condition. With the used pyrolysis condition, elimination of functional groups and the release of small molecules are insufficient for the formation of a highly porous architecture and large surface area. In the following, the biomass was pyrolyzed with the help of NaOH (Fig. 1b & e) and SP (Fig. 1c & f). Visibly, these particles are broken down into smaller pieces with concave features and microcavities on the surface of the produced activated carbons (ACs). The obvious changes are due to the activation process, which also suggests that SP would etch the carbon skeleton under the same pyrolysis condition (Fig. 1g). Compared to hemicellulose-derived carbon (Fig. 1e & f), the morphologies of the lignin-derived carbon (Fig. 1b & c) are nearly unchanged, which is mostly due to the relatively robust carbon skeleton.
The traditional NaOH acts as a strong oxidizing agent at high temperature, promoting the removal of carbon atoms and the development of nanocavities. However, it is a highly corrosive and would generate a high level of heat as it dissolves during the pre-treatment and post-treatment procedure. Moreover, the strong base could induce chain breaking for lignin and hemicellulose, and lead to an incapability to control the pyrolysis. Fig. S3† shows the characteristics of the biomass and their aqueous mixtures. The NaOH-catalyzed cleavage of aryl ether bonds in both lignin and hemicellulose leads to chain scission, improved water solubility, enhanced viscosity, and darkened color.38 Additionally, the mixing of the precursor and a strong base produces extreme heat (∼70 °C), and could induce high operation risk. In contrast, the mixing of the precursor and SP molecular salt leads to almost no heat (∼25 °C) and allows for safe pre-treatment. Moreover, the chain scission of biomass might not occur as the viscosity of the mixture merely changed. Such behavior makes SP an effective and harmless reagent in producing microporous carbons.
Based on the nitrogen adsorption and desorption isotherms in Fig. 2a, the surface areas of SHLC, SHHC, SPLC and SPHC are calculated to be 374.8, 405.3, 249, and 1217.9 m2 g−1, respectively (Table S1†). Although typical type IV hysteresis features have been observed, the four carbons are micropore-dominated, conferring to the pore distribution curves (Fig. 2b). The skeleton structure and composition of porous carbon are also essential for the electrochemical performance. In Fig. 2c, all carbons exhibit two broad characteristic peaks centered at ∼23.1° and ∼45°, which are attributed to the [002] and [100] planes of the carbon skeleton structure.39 The result demonstrates the amorphous disorder of the carbons with large amounts of defects. In Fig. 2d, the D band (∼1350 cm−1) and G band (∼1590 cm−1) are presented, ascribed to the defective graphitic structure and packed graphitic layers, respectively.40 The ratios of ID/IG are calculated based on the peak intensities, which reflect the defects and disordered structures in the porous carbon. All carbons show ID/IG in the range of 0.8–0.84. Considering that cellulose chains experience more severe thermal cleavage and elimination of pyranose rings, this contributes to the aromatic condensation and slightly enhanced long-range stacking in the hemicellulose-derived carbon (HC). The addition of NaOH and SP induce further reactions at high temperature, and thus leads to more defects and disordered structures. The high level of aromaticity in lignin contributes to the resistance to thermal cleavage, requiring more energy for the preferential formation of the stacking structure and structure arrangement.40 It could be understandable that the addition of activation reagents results in a smaller effect on the defects of the lignin-derived carbons.
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Fig. 2 (a) Nitrogen isotherms, (b) pore distributions, (c) XRD patterns, (d) Raman spectra, (e) XPS survey curves, and (f) high-resolution N 1s spectra of the produced carbons. |
The dopants can promote the adsorption of the electrolytes and provide extra pseudocapacitive reactions, and thus lead to favorable electrochemical kinetics and performance.41 All biomass and mixtures allow the formation of oxygen-doped ACs after the pyrolysis process (Fig. 2e). This is due to the presence of rich oxygen-containing functionalities. Moreover, SPLC and SPHC carbons show extra nitrogen dopants that were inherited from SP molecules (Fig. 2f and Table S1†). Herein, the cyclic and conjugated SP molecules not only act as an activation reagent, but also as a source of carbon skeleton building block. The TGA curve reveals that SP has a high sublimation temperature and high retention (>40 wt%) at 800 °C (Fig. S2c†). Therefore, it is proposed that SP could fuse with degraded biomass species at the aromatization stage during the co-pyrolysis process, rendering the randomly stacked doped graphite layers. Meanwhile, the sodium counter-ions decomposed into sodium species, which activated the graphite layer and create microcavities and defect structures. To further investigate the composition, SP was mixed with an equal mass of SPLC or SPHC for a second co-pyrolysis. It is found that the additional SP treatment in both cases apparently increases the surface nitrogen and sulfur contents (Fig. S4 and Table S1†). The result indicates that the doping mechanism is also applicable to carbon. Additional treatment of SPLC or SPHC with the SP molecular salt further influences the defects and carbon structures, as evidenced from the increased ID/IG ratios and shifted [002] planes (Fig. S5†). However, the high-temperature fusing of SP derivatives with microporous carbon blocks the micropores, and leads to decreased surface areas of ACs (Fig. S6†).
Next, carbon cathodes were prepared and assembled into ZICs for electrochemical analysis. Fig. 3a and Fig. S7† show the cyclic voltammetry (CV) profiles of ZICs measured in 2 M aqueous ZnSO4. The cathodes show approximate rectangular shapes with a few redox bumps, indicating the feature of the electric double-layer capacitive behavior and the presence of surface faradaic behavior. Moderate good rate performance can be achieved because satisfactory shapes are retained at faster scan rates (Fig. S7†). Among those cathodes, LC and HC cathodes show extremely small CV areas due to limited surface areas. The SPHC cathode shows the largest area at the same scanning rate, ascribed to the large surface area and heteroatoms. However, it is found that the enhanced heteroatoms but with reduced surface areas render the cathodes (SP2LC and SP2HC) with inferior electrochemical performance (Fig. S7†). Thus, more calculations and measurements are conducted to comprehend the best performance of the SPHC cathode. In Fig. 3b, the intrinsic kinetics of the carbon cathodes is analyzed based on CV profiles using Dunn's method.29 The capacitive contributions continually increase with the increase of scan rates. It is also noted that NaOH-activated carbon cathodes show an overall larger capacitive performance compared to the SP-activated carbon cathodes. It is believed that co-pyrolysis of SP and biomass provides oxygen/nitrogen/sulfur dopants and tortuous pathways at the same time, which restricts the rate of charge transportation. Nevertheless, SPHC shows relatively good capacitive contribution of 45%, 48%, 55%, and 79% at scan rates of 5, 10, 25, and 100 mV s−1, respectively. The results suggest the fast kinetics and redox process in the SPHC cathode.
Galvanostatic charge–discharge (GCD) measurements have also been carried out (Fig. S8†). The profiles at different current densities exhibit nearly triangular shapes, supporting its good electric double-layer characteristic. Fig. 3c shows the derived voltage-capacity profiles of four ACs at 1 A g−1. SPHC delivers a high capacity of 94.9 mA h g−1, beyond that of SHHC (51.2 mA h g−1), SPLC (44.2 mA h g−1), and SHLC (39.1 mA h g−1), at the same current density. The performance of SPHC is comparable to most reported studies, ZnLFK-PC,28 AC,42 CSMCs,43 N-HPC,44etc. Fig. 3d presents the rate performance in the current densities of 0.5–10 A g−1. SPHC has a favorable capacity retention of 45.8%, which is higher than that of SHHC (39.8%), SPLC (24.4%), and SHLC (30.7%). Besides, the highest capacity of 108.6 mA g−1 is achieved on the SPHC cathode at a lower current density of 0.5 A g−1, ensuring the highest energy density of 67.8 W h kg−1 (Fig. 3e). Owing to the high surface area and suitable dopants, SPHC possesses excellent electrochemical performance. Electrochemical impedance spectroscopy (EIS) technique has been used to illustrate the resistance properties of the cathodes. The Nyquist plots first demonstrate that all cathodes experience small, similar electrode resistances (10–12.5 Ω) (Fig. 3f). At high frequencies, the electrolyte resistance values are determined to be about 40 Ω, 85 Ω, 90 Ω, and 135 Ω for SPHC, SHHC, SPLC, and SHLC, respectively. The SP-derived ACs show smaller electrolyte resistance compared to the NaOH-derived ACs. Although the pack structure of cathode influences the resistance, it is believed that the oxygen/nitrogen/sulfur dopants lower the surface energy and enhance the surface electrolyte wettability, resulting in smaller interfacial resistance.28 Meanwhile, the dopants and tortuous pathways associated with SP-derived ACs affect the charge diffusion and capacitive behavior, resulting in slow slopes or more Warburg-like feature at medium frequencies. The resistance properties agree well with their electrochemical properties and certify the well-performed SPHC cathode.
Fig. 4adisplays the cycling performance of SPHC-based ZIC. To better investigate the electrochemical behavior on the SPHC cathode, zinc foils are often replaced to exclude the influence of the anode on ZIC. Moreover, the cycling measurement was paused randomly for 25 times (∼250 h of total break time) and ran under fluctuating temperatures to record the result that mimics practical use condition. As a result, after 20000 cycles at 7 A g−1 (∼280 h), the device still maintains a high-capacity retention of 85.9% and nearly ∼100% coulombic efficiency, demonstrating excellent cycling stability. Moreover, it is noted that the temperature shows a positive correlation effect on the capacity retention. This is possibly due to the enhanced charge transport at elevated temperatures. After cycling, the resistance property was evaluated by EIS (Fig. 4b). The electrode resistance and electrolyte resistance increase from 10 Ω to 17.8 Ω and from 40 Ω to 73.7 Ω, respectively, whereas the Warburg-like feature remains close. Evidences exist on the dynamic performance of the SPHC cathode on ZIC, despite the electrode structure being supposedly stable at the conducted electrochemical condition. The occurrence of the faradaic redox reaction, electrolyte, and the effect of temperature fluctuation could be considered to play a role in the cathode structure reconstruction,22 leading to the reduced capacity retention. The self-discharge performance describes the long-term charge storage properties of the ZIC. In Fig. S9,† the open-circuit voltage of SPHC-ZIC has been monitored. Although the voltage drops rapidly from 1.80 V to 1.44 V during the first 20 h, high voltage retention values (∼1.38 V) have been observed during the next 100 h. The slow self-discharge rate is comparable with reported work,45 and the result demonstrates the superior anti-self-discharge performance.
Morphologic and elemental analyses were performed on the SPHC cathodes, and the results are presented in Fig. 4(c–e). Generally, discharging from a high voltage to low voltage would lead to the formation of a zinc complex. Therefore, this will increase the Zn species on the surface of the cathode. Upon charging, the reverse process occurs. The H+ ions are proposed as the major intermediates for cathode reconstruction via precipitation-redissolution of complex zinc hydroxides.22,46,47 Here, the operando techniques experimentally confirm the electrochemical process and mechanism. In Fig. 4c, the EDX quantitative analysis on the fresh SPHC cathode first shows the decrease of the Zn/C ratios (from 0.27 to 0.09, and to 0.03) and then shows the increase of Zn/C ratios (from 0.03 to 0.10 and to 1.27) during charging and discharging. Accordingly, in Fig. 4d, the gradual dissolution and then reformation of the zinc complex during charging and discharging have been identified. Although the cycled SPHC cathode displays the same mechanism, i.e., the Zn/C ratios decrease from 6.69 to 4.79 and to 1.86 upon charging and the ratios increase from 1.86 to 4.56 and to 10.11 upon discharging, the ratios are extraordinarily high. In particular, the Zn/C ratio at 1.8 V is much higher than 0, indicating the presence of a large quantity of the Zn species. This also means that the intermediates do not react stoichiometrically. The feature can also be recognized from the morphologies shown in Fig. 4e, where large zinc complex-based flakes exist at all states (including the state at 1.8 V). Partial degradation of the surface-active functionalities under long-term electrochemical measurement leads to an inequivalent stoichiometric reaction between the intermediates and electrolyte. Therefore, the flakes reside on the cathode at 1.8 V.48 Moreover, it is believed that the numerous crystal precipitation-redissolving repeats drive the reconstruction of the cathode structure, possibly by modifying the original configurations, breaking the conductive junctions, engulfing the active sites, blocking cavities, etc.,48,49 thus resulting in the capacity loss during cycling.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4gc02429j |
This journal is © The Royal Society of Chemistry 2024 |