Open Access Article
Yingna Chang‡
a,
Qidong Dang‡b,
Imran Samoa,
Yaping Lia,
Xuejin Lib,
Guoxin Zhang
*b and
Zheng Chang
*a
aState Key Laboratory of Chemical Resource Engineering, Beijing University of Chemical Technology, Beijing, 100029, China. E-mail: changzheng@mail.buct.edu.cn
bCollege of Electrical Engineering and Automation, Shandong University of Science and Technology, Qingdao 266590, China. E-mail: zhanggx@sdust.edu.cn
First published on 24th January 2020
The removal of heavy metal contaminants has aroused global attention due to water shortage and the lax control on the discharge of heavy metal pollutants. Capacitive deionization (CDI) has emerged as a robust, energy-/cost-efficient technique for water treatment. Herein, we reported the simple synthesis of N, S-co-doped carbon materials (NS-C) derived from PVC plastic wastes as CDI electrode materials for the efficient removal of heavy metal ions (HMIs). The NS-C exhibited a large specific surface area (∼1230 m2 g−1) and contained heavy heteroatom doping (∼4.55 at% N and ∼13.30 at% S). The CDI electrode fabricated using NS-C showed high removal efficiency (94–99%), high capacity (36–62 mg g−1), and good regeneration capability for the adsorption of various kinds of low-concentration heavy metal ions (including Fe2+, Co2+, Ni2+, Cu2+, Pb2+, and Cd2+). Moreover, PVC plastic wastes that are heavily accumulated in the environment and extremely hard to be decomposed and recycled were applied as the carbon source in this study for the fabrication of NS-C, which further rendered the importance of our study in practically treating hazardous waste (HMIs) with waste (PVC plastic wastes) in a clean and efficient way.
Carbon-based electrode materials for CDI are promising options in terms of their wide availability at low costs.2,3,22 In particular, many natural products, such as glucose,29,30 sucrose,31–33 and cellulose,34,35 can be used as carbon sources to fabricate carbonaceous materials. In order to gain carbon materials with a higher adsorption capacity, it is applicable and feasible to involve heteroatom doping to provide more anchoring sites for metal ions.36,37 Common strategies for incorporating heteroatom species into carbon materials are mainly based on the pyrolysis of organics that contain heteroatom sources. However, these inevitably generate hazardous volatile organic compounds and lead to uncontrollable doping types and contents.37
Recently, a simple and effective dehalogenation strategy for fabricating doped carbon materials under mild conditions was developed.17,39–42,52–54 For instance, over 10 at% nitrogen can be incorporated into the as-formed carbon at room temperature under simple hand grinding.17 The ultrahigh doping efficiency is mainly due to the high reactivity of dehalogenated carbon sites that are capable of fast coupling with adjacent atoms.43 Polyvinyl chloride (PVC) is one sort of widely applicable halogenated polymer in daily life, but is extremely hard to decompose and recycle due to its extremely stable physico-chemical properties. Currently, the severe PVC accumulation has caused irreversible damage to our environment.44–47 It is of significance and practicality to fabricate doped carbon materials from PVC and explore their CDI applications.
Here in this study, we managed to fabricate a N, S-co-doped carbon material (NS-C) by dehalogenating PVC plastic wastes using KOH in the presence of thiourea (N/S dopant). It was characterized that 4.55 at% N and 13.30 at% S were doped in the resulting NS-C. Meanwhile, the NS-C is highly porous and contains a multi-scale hierarchical pore (macro-/meso-/micro-pores), achieving a high specific surface area of 1230 m2 g−1. The NS-C, once fabricated into the CDI electrode, exhibited very high removal efficiency (94–99%), high capacity (36–62 mg g−1), and good regeneration performance towards capacitive adsorbing of various kinds of low concentration HMIs. CDI measurements showed that NS-C presented a larger affinity and capacity for HMIs over alkali metal ions and alkali earth metal ions due to the heavy heteroatom doping. Moreover, the dehalogenation route of applying PVC plastic wastes as a carbon source to synthesize CDI electrode materials may potentially open up clean, efficient disposal and prosperous utilization of annoying PVC plastic wastes, which is a worthwhile “kill two birds with one stone” strategy to control waste by waste.
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5 in 2.0 mL ethanol and thoroughly sonicating to reach a homogenous slurry. Then, the viscous slurry was uniformly coated on a graphite paper (size: 6.0 cm × 7.0 cm × 0.2 mm) and dried in an oven at 80 °C overnight. In a typical CDI measurement, 100.0 mL aqueous solution with an initial metal ion concentration of 50 ppm (FeCl2, CoCl2, NiCl2, CuCl2, PbCl2, or CdCl2) in a beaker was continuously fed into the CDI unit using a peristaltic pump with a constant flow rate of 25.0 mL min−1 and the effluent was returned to the beaker. Meanwhile, the applied voltage was 1.5 V for adsorption and −1.5 V for desorption. The concentration of solution was monitored by a conductivity meter (Type 308F, Leici Company) located at the outlet of the CDI unit (as schemed in Fig. S1†). As shown in Fig. S2,† there is a linear relationship between the conductivity of the solution and the concentration of metal ions. In order to measure the selectivity, a 100.0 mL mixture solution containing 20 ppm Mg2+, 20 ppm Ni2+, and 20 ppm Pb2+ was used. After CDI treatment, the final concentrations of three metal ions were measured by an inductively coupled plasma-atomic emission spectrometer (Thermo, ICP-6300).
The adsorption capacity of heavy metals (W) was calculated by the following eqn (1):
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| Fig. 1 (A) Fabrication scheme for NS-C from PVC plastic waste. (B) SEM and (C) TEM images of PVC-derived NS-C. (D) Organic elemental analysis of N-C, S-C, and NS-C. | ||
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| Fig. 2 (A) XRD spectra and (B) Raman spectra of RT-NS-C and NS-C. (C) N2 absorption/desorption curves and (D) pore size distribution curves of N-C, S-C, and NS-C. | ||
As revealed in Fig. 2B, there were two distinct Raman bands presented for both RT-NS-C and NS-C. The bands of NS-C located at ∼1346 and ∼1604 cm−1 could be unambiguously indexed to the D and G bands for graphitic carbon materials, respectively.50 Meanwhile, RT-NS-C exhibited a set of bands consisting of two sharp bands but the bands were heavily blue-shifted to ∼1127 and ∼1519 cm−1, confirming that RT-NS-C is highly carbonized.43 The pore type of NS-C, as revealed by N2 adsorption/desorption curves (Fig. 2C), could be indexed to a combination of type-I and type-II pores, which suggests that huge amounts of micropores and a small proportion of mesopores and macropores exist.38 Due to similar protocols, the control samples of N-C and S-C exhibited similar N2 adsorption/desorption curves. The specific surface areas (SSA) of NS-C, N-C, and S-C were 1230, 1029, and 989 m2 g−1, respectively. Fig. 2D displays their pore distribution curves, revealing the overwhelmingly present micropores in all three samples. The minor amount of mesopores (Φ ∼ 2–10 nm) were mainly introduced by the rapid removal of gas bubbles and KOH activation.48
XPS measurements were employed to characterize the surface composition of NS-C. There were mainly four types of elements present in NS-C: carbon (C 1s, ∼285 eV), oxygen (O 1s, ∼532 eV), nitrogen (N 1s, ∼400 eV), and sulphur (S 2p, ∼164 eV), as shown in Fig. 3A. Deconvolution was performed on each element for detailed bond configurations. In the C 1s spectra (Fig. 3B), it was revealed that over 25.6% carbon atoms were connected to non-carbon atoms, including O, N and S, which is further evidenced by the ultrahigh content of heterodoped elements. As shown in the S 2p spectra (Fig. 3D), S and C connections could be sorted into three types: C–S single bond, C
S double bond, and oxidized S bound to C. The considerable amount of oxidized S in the carbon matrix was probably due to the KOH activation and oxidation during the high-temperature treatment. N 1s spectra (Fig. 3C) indicated that the N species mainly existed in a pyrrolic and graphitic N forms, accompanied by negligible amount of pyridinic N. The ultrahigh content of alien species was further confirmed by organic elemental analysis, reaching 27.8 at% (combining O, N, and S), which provided abundant sites for anchoring metal cations.
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| Fig. 3 (A) The XPS survey, (B) C 1s, (C) N 1s, and (D) S 2p XPS spectra of NS-C and their deconvoluted curves. | ||
Therefore, the as-made samples were fabricated into electrodes for supercapacitor measurements in aqueous Na2SO4 solution (1.0 mol L−1) prior to the CDI tests. As shown in Fig. 4A and S5A–C,† all the CV profiles of the as-obtained materials exhibited a near-rectangular shape, suggesting that the electrochemical double-layer capacitive behaviour dominated all three samples. Among them, the NS-C showed the largest area, meaning more charge was capable of being stored in NS-C than in N-C and S-C, which was possibly due to its higher degree of doping and synergistic effect of dual N, S doping.48 As measured by galvanic charge/discharge (Fig. 4B and S5D/E†), the NS-C sample delivered a very high capacitance of 290.2 F g−1 (at 1.0 A g−1) in Na2SO4 aqueous solutions, which is superior to that of N-C and S-C. Remarkably, the NS-C was able to maintain over 70.3% of capacitance during charge/discharge at a high rate of 20.0 A g−1 (Fig. 4C and inset of Fig. 4D). As shown in Fig. 4D, over 96.7% capacitance of the NS-C could be kept after high-rate cycling for 5000 times at a current density of 5.0 A g−1, implying that the NS-C was electrochemically stable under the measurement conditions in a concentrated alkaline solution. All in all, we managed to exploit the supercapacitor application of PVC waste-rendered porous N, S-co-doped carbon materials.
Furthermore, the NS-C material, having a large SSA, open porous structure, high-content heteroatom doping, and large specific capacitance, was submitted to HMI removal tests using a bench-scale capacitive deionization (CDI) apparatus consisting of a pump, a conductivity meter, an electrical power supply, a self-made CDI unit, and a feed water reservoir (Fig. S1†). The conductivity change is closely related to the ion concentration in solution, which helps in monitoring the adsorption/desorption processes of ions.36 Normally, single-element doping in carbon materials such as N or S provides robust sites for ions to anchor. Herein, the as-fabricated NS-C provided much more heteroatom doping sites than single N or S doped carbon materials, as shown in Fig. 1D. Initially, a voltage was not applied to reveal the extent of physical adsorption. It was observed that the system conductivity exhibited a negligible conductivity decrease in the first 20 min (Fig. 5A), meaning that the physical adsorption with the circumstance of no applied voltage was not prominent. Upon voltage was applied, the conductivity for each testing system was observed to sharply drop. The comparison of the deionization curves of NS-C and two control samples (N-C and S-C) for Fe2+ is displayed in Fig. 5A/B. It was confirmed that the co-doped carbon materials (NS-C) exhibited a superior deionization capacity and faster deionization rates than that of the other samples with single-element doping. The significant improvement of NS-C in the removal of HMIs could be attributed to the large accessible SSA and deeply activated carbon surface by the introduction of rich heteroatom doping sites.
The standard curves of conductivity versus concentration for different metal ions are plotted in Fig. 5C. The applied voltage (1.5 V) was used in the adsorption process and the voltage was reversed (−1.5 V) in the desorption process. Due to the difficulty in treating low-concentration HMIs, the deionization performance was investigated in 50 ppm HMI solutions including Fe2+, Co2+, Ni2+, Cu2+, Pb2+, and Cd2+. Prior to all CDI measurements, we first recorded the pH variations of a 50 ppm Fe2+ solution during the CDI measurements in Fig. S6.† The initial pH of the solution was ∼5.75 and along with the CDI process of absorbing Fe2+, the pH value gradually increased to 6.23 at the end of the CDI, suggesting that the pH had limited fluctuation. Meanwhile, there was no obvious redox peak of NS-C in the 50 ppm Fe2+ solution under a scan rate of 5 mV s−1 (Fig. S7†), implying a dominating electrochemical double-layer capacitive behaviour against faradic reactions. Upon the voltage was applied, it was forced to reach a close-to-zero conductivity threshold for the cases of Cu2+, Pb2+ and Ni2+ over 210 min (Fig. 5C). The final ion concentrations calculated from the corresponding conductivity at 210 min were reduced to 5.8, 3.7, and 9.2 ppm for Ni2+, Pb2+, and Cu2+ from 50 ppm, respectively. The removal capacities for Fe2+, Co2+, Ni2+, Cu2+, Pb2+ and Cd2+ as calculated from deionization curves were 56.3, 56.4, 55.2, 51.0, 57.9 and 36.6 mg g−1, respectively (Fig. 5D). The significance in the adsorption rate constants for different cations may arise from their different affinity with heterodoping atoms.17,20,22 Such high removal capacities for various heavy metal cations surpassed most current reported values applying CDI techniques (Fig. 5E).17,22,49–51
The regeneration capability of CDI electrode materials is another important aspect for practical applications. Capacities and efficiencies of deionizing heavy metal ions after the adsorption equilibrium using the NS-C electrode in different cycles were investigated and recorded. As shown in Fig. 5F and S8,† over five consecutive adsorption/desorption cycles for 50 ppm Fe2+ revealed that the system conductivity was recoverable with voltage converting and the deionization efficiency for all cycles was above 99%, indicating a high efficiency and remarkable stability of the NS-C electrode, which was probably related to the negligible physical adsorption.
We further explored the capability of NS-C to selectively adsorb HMIs over low toxicity metal ions in a mixed solution. Fig. S9† shows the deionization curve of NS-C using a CDI system in a mixed ionic solution containing 20 ppm Mg2+, 20 ppm Ni2+, and 20 ppm Pb2+. While being monitored, the conductivity of the mixed solution took a sharp decrease in the first 60 min and finally reached a plateau. For exactly measuring the removed ions, the mixed solutions were submitted to ICP measurements before and after the CDI process at 210 min. Though the starting concentrations for each type of ion were all 20 ppm, after CDI, it was exciting to find that nearly all HMIs had been removed from the mixed solution while only ∼6.7 ppm Mg2+ was left. Therefore, NS-C held a larger affinity and capacity for HMIs over less hazardous alkali metal ions and alkali earth metal ions, which might be attributed to the huge amount of cooperative heteroatom doping in the electrode materials. For a real CDI system, it is not possible to completely remove all the ions in solution. However, there is a significant difference in the achievable adsorption thresholds when using different electrode materials. As is well known, the removal of very low concentrations of HMIs is still a challenge. Herein, the concentration of Co2+ decreased to 1 ppm to study the removal capacity of NS-C electrode materials using the CDI technique. As shown in Fig. S10,† the removal efficiency rapidly reached 57.8% in 30 min and finally 82.6% in equilibrium.
Footnotes |
| † Electronic supplementary information (ESI) available: The scheme of an integrated capacitive deionization apparatus; additional electron microscopy images of N-C, S-C, and NS-C; XRD profiles of N-C, S-C, and NS-C; supercapacitor characterizations of NS-C; CDI cycling stability measurements of NS-C. See DOI: 10.1039/c9ra09237d |
| ‡ These authors contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2020 |