Danfeng Qin†
ae,
Ruiyu Xu†ae,
Hangjia Shenae,
Xamxikamar Mamata,
Le Wangae,
Shanshuang Gaoa,
Ying Wangae,
Nuerbiya Yalikunae,
Thomas Wagberg*b,
Shiguo Zhangc,
Qunhui yuan*d,
Yongtao Lia and
Guangzhi Hu*ae
aKey Laboratory of Chemistry of Plant Resources in Arid Regions, State Key Laboratory Basis of Xinjiang Indigenous Medicinal Plants Resource Utilization, Xinjiang Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Urumqi 830011, Xinjiang, China. E-mail: guangzhihu@ms.xjb.ac.cn
bDepartment of Physics, Umea University, 90187 Umea, Sweden. E-mail: thomas.wagberg@umu.se
cDepartment of Chemistry and Biotechnology, Yokohama National University, 79-5 Tokiwadai, Hodogaya-ku, Yokohama 240-8501, Japan
dHarbin Institute of Technology, Shenzhen 518055, China. E-mail: yuanqunhui@hitsz.edu.cn
eUniversity of Chinese Academy of Sciences, Beijing 100049, China
First published on 25th July 2017
Nitrogen-doped mesoporous carbon (NMC) derived from a single small-molecule protic salt (p-phenylenediamine bisulfate) is used for sensing toxic heavy metal ions. Using Nafion, bismuth and NMC to anchor the glassy carbon electrode surface, the fabricate electrode shows high sensitivity for detecting Cd(II) and Pb(II). The limits of detection (S/N = 3) are estimated to be 0.3 μg L−1 for Cd(II) and 0.4 μg L−1 for Pb(II), respectively, which are 10 and 25 times lower than the maximum acceptable content for drinking water recommended by the WHO. Furthermore, the sensor is successfully used to analyze Cd(II) and Pb(II) in tap-water with high anti-interference capability and good recovery.
Nitrogen-doped mesoporous carbon (NMC) has shown excellent physical and chemical properties, such as abundant pore structure, large surface area, and low density,7 making it frequently applied in lithium batteries,8 fuel cells,9 supercapacitors,10 catalyst supports,11 separation processes12 and sensing.13 To detect heavy metals, NMC is hypothesized to exhibit remarkable performance because the mesoporous structure not only provides efficient diffusion and mass transfer for heavy metal ions, but also contains a large amount of electron-donating nitrogen atoms which can improve the performance of sensor.14,15 For example, Cui et al. demonstrated a nitrogen-doped porous carbon was synthesized with Al-based organic gel template for detection of Cd(II) by ASV with good stability and excellent selectivity.16
Normally, mesoporous carbon is produced based on the sacrifice template method, but the method is multistep, and time-consuming.7,17–19 For example, Shen et al. recently reported a MgO/ordered mesoporous carbon composite that could be applied for determination of Pb(II).20 The casting template method used for the preparation of ordered mesoporous carbon is complex, including SBA-15 (as template) preparation, infiltration of the sucrose into the SBA-15, carbonization of the sucrose, and finally etching of the silica template.
Nitrogen-doped porous carbon is commonly prepared in two ways: in situ synthesis or a post-treatment functionalization. The former method results in a homogeneous distribution of N,15 while with the latter it is difficult to control the nitrogen content and there is a risk of blocking the porous architecture.21 Xiao et al. successfully prepared nitrogen-doped microporous carbon with 25.0 at% nitrogen content for detection of Cd(II) and Pb(II) by in situ doping of nitrogen.22
In summary, traditional methods for the synthetic of NMC materials are typically tedious and time-consuming, therefore we describe a facile one-step template-free method to prepare NMC via carbonization of a protic salt ([pPDA][2HSO4]),19 which behaves as an carbon and nitrogen source during pyrolysis. We then use the prepared NMC in an electrochemical heavy metal sensor. The synthetic action of Nafion and bismuth on the NMC makes the sensor highly sensitive, and we show that it can be probed by simultaneous detection of Cd(II) and Pb(II).
The morphology of NMC was characterized by a field emission scanning electron microscope (SEM, Carl Zeiss, Oberkochen, Germany). X-ray photoelectron spectra (XPS) were recorded with an Axis Ultra DLD electron spectrometer (Kratos Analytical Ltd., Manchester, UK). The structure analysis of NMC was operated on JEOL-2100F microscope (JEOL, Tokyo, Japan) at 200 kV. N2 adsorption–desorption isotherms was determined with an Autosorb-IQ-MP gas sorption analyzer (Quantachrome Instruments, Boynton Beach, Florida USA). The content of Cd(II) and Pb(II) was measured with Inductively Coupled Plasma-Mass Spectrometry (ICP-MS, ELAN DRC II, PerkinElmer, USA).
The electrolyte (10 mL) included acetate buffer (0.1 M, pH = 5.0) and the target metal ions. If the modified electrodes need to deposit Bi film, 400 μg L−1 Bi(III) is added into the electrolyte. Under optimized conditions, differential pulse anodic stripping voltammetry (DPASV) was applied for heavy metals determination. The accumulation step was set at −1.1 V under stirring for 420 s. Following the preconcentration, the solution was kept quiet for 10 s. Then the DPASV curve was recorded at differential pulse mode from −1.0 V to −0.4 V.
Fig. 1 (a) SEM and (b) TEM image of NMC, (c) the relative N2 sorption isotherms (inset: pore width distribution of NMC), and (d) XPS (inset: high-resolution N 1s spectrum). |
The pore structure of NMC was explored by nitrogen adsorption–desorption experiments. As presented in Fig. 1c, a hysteresis loop at pressures P/P0 > 0.5 is observed, which indicates the presence of mesopores. The BET surface area is calculated to be up to 596 m2 g−1 with a narrow pore-size distribution and an average pore size of 7.0 nm as shown as in the inset of Fig. 1c.
To investigate the chemical valence and elemental composition of the NCM, XPS measurement was performed in the region from 0 to 600 eV. The elemental content of NMC is determined to 84.2 at% for C, 10.0 at% for N, 5.0 at% for O, and 0.9 at% for S (Fig. 1d). The high resolution N 1s spectra of NMC (inset in Fig. 1d) could be deconvoluted into four peaks, at 397.80, 400.08, 402.16, and 405.05 eV, which correspond to pyridine-like, pyrrole-like nitrogen as well as oxidized species at higher binding energies (>402 eV),24–26 respectively. The XPS results clearly prove that N atoms have been successfully doped into the material. N introduction can accelerate the electron transfer and improves the sensitivity of the modified electrode.27
The electrochemical behaviors of Nafion–GCE (curve a), Bi/GCE (curve b), Nafion–Bi/GCE (curve c), OMC–Nafion/GCE (curve d), NMC–Nafion/GCE (curve e), and NMC–Nafion–Bi/GCE (curve f) were investigated by DAPSV in HAc–NaAc (0.1 M, pH 5.0), respectively. As presented in Fig. 2, there are two peaks around −0.8 V and −0.6 V, corresponding to the stripping peak of Cd and Pb at these six electrodes. The anodic peak currents of Cd and Pb at Bi/GCE are 5.09 μA and 6.31 μA, which is almost 45.5% and 64.3% at the NMC–Nafion–Bi/GCE. Compared to Nafion/GCE, the Nafion–Bi/GCE shows a clear increase in peak currents, ascribed to the ability of the Bi-film to form a fused alloy with Cd and Pb (Cd(II) + Bi(III) + 5e → Cd–Bi,Pb(II) + Bi(III) + 5e → Pb–Bi).28 Additionally, the stripping peak currents of Cd(II) and Pb(II) at NMC–Nafion/GCE are higher than OMC–Nafion/GCE, which suggests that NMC shows more outstanding analytical performance in determination heavy metals than OMC. Moreover, the peak current of NMC–Nafion–Bi/GCE improves about 47% for Cd(II) and 66% for Pb(II) than that of Nafion–Bi/GCE, respectively. These improvements in peak current can be attributed to the porous structure and large surface area of the NCM, which is beneficial for an effective accumulation of heavy metal ions.
The effect of Bi(III) concentration was examined from 100 μg L−1 to 600 μg L−1. As shown in Fig. 3a, the stripping peak currents of Cd(II) is gradually decreased when the Bi(III) concentration was higher than 400 μg L−1 and Pb(II) concentration is higher than 500 μg L−1. Thus, we chose 400 μg L−1 Bi(III) as the optimum concentration.
The influence of deposition potentials on the DPASV signals of Pb(II) and Cd(II) was explored in the potential window from −0.9 to −1.3 V. The results displayed in Fig. 3b indicate that the stripping peak currents increase sharply when the accumulation potential is shifted negatively from −0.9 to −1.1 V, and the maximum current for these two ions are at −1.1 V and then shift further in the negative direction when the deposition potential is further decreased. This phenomenon is ascribed to the significant hydrogen evolution at more negative potentials.29 Here −1.1 V is selected as the optimized deposition potential.
Solution pH can also affect the DPASV peak current of the Cd(II) and Pb(II) oxidation. Fig. 3c presents the influence of buffer pH on the DPASV responses of Cd(II) and Pb(II). When the pH increases from 4.0 to 5.0, both stripping peak currents increase, while a further increase in pH leads to a decrease in stripping signal. This is ascribed to the formation of metal hydroxide complexes.1 Therefore, a pH 5.0 was applied in this work.
Accumulation time is a really important parameter to heavy metal detection by using DPASV method. It can be seen from Fig. 3d, the influence of the accumulation time on detection of Cd(II) and Pb(II) was investigated from 180 to 480 s. The stripping signals increase gradually to the deposition time from 180 up to 420 s. However, when the preconcentration time is beyond 420 s, the stripping peak currents almost remain constant due to the rapid surface saturation.30 In order to get high peak current, an accumulation time 420 s is chosen for further study.
Under the optimized experimental conditions, NMC–Nafion–Bi/GCE was applied in the successive analysis of Cd(II) and Pb(II) in the range from 4 μg L−1 to 130 μg L−1. DPASV response signal (vs. Ag/AgCl) for different concentrations of target metal ions and the relative calibration plots were illustrated in Fig. 4b and c. The analytical curves both for Cd(II) and Pb(II) cover two linear ranges from 4 to 10 μg L−1 and from 10 to 130 μg L−1, demonstrating the good linearity of the proposed sensing electrode for both Cd(II) and Pb(II). The regression equation of Cd(II) and Pb(II) are listed in Table 1. As seen from the Table 1, the slop of the linear in the low concentration range is much smaller than the one in the high concentration range. It could be due to the difference in rate determining step in these two concentration ranges. Moreover, the limit of detection (at S/N = 3) were valuated to be 0.3 μg L−1 for Cd(II) and 0.4 μg L−1 for Pb(II), which are 10 times for Cd(II) and 25 times for Pb(II) lower than the reference value of drinking water given by WHO (Cd: 3 μg L−1, Pb: 10 μg L−1),32 making the NMC–Nafion–Bi/GCE to a good candidate for the analysis of real aqueous samples.
Heavy metals | Regression equation (y: μA, x: μg L−1) | LOD (μg L−1) | Maximum acceptable content (μg L−1) | |
---|---|---|---|---|
Linear range I: 4–10 (μg L−1) | Linear range II: 10–130 (μg L−1) | |||
Cd(II) | y = 0.179x − 0.550, R2 = 0.990 | y = 0.218x − 0.446, R2 = 0.997 | 0.3 | 3 |
Pb(II) | y = 0.081x + 0.165, R2 = 0.999 | y = 0.198x − 0.934, R2 = 0.999 | 0.4 | 10 |
The sensing performance of NMC–Nafion–Bi/GCE towards Cd(II) and Pb(II) is compared with the other reported sensors and presented in Table 2. It is obvious that the proposed NMC–Nafion–Bi/GCE is comparable to the previously reported results.
Modified electrode | Method | Range in μg L−1 | Limit of detection in μg L−1 | Deposition time in s | Ref. | ||
---|---|---|---|---|---|---|---|
Cd | Pb | Cd | Pb | ||||
a Nitrogen doped microporous carbon derived from ZIF-8.b Multi-walled carbon nanotube.c Poly(pyrocatechol violet).d Graphene.e Mercury film electrode.f Dibenzo-24-crown-8.g Screen-printed carbon electrode.h Screen-printed electrode.i Electroreduced graphene oxide.j Thionine.k 2-Mercaptoethanesulfonate.l 2,5-Dimercapto-1,3,4-thiadiazole.m Polyaniline.n Bismuth-oxychloride.o Poly(2,5-dimercapto-1,3,4-thiadiazole). | |||||||
aCarbon of ZIF-8/Nafion/Bi/GCE | DPASV | 2–100 | 0.5–100 | 1.5 | 0.05 | 180 | 22 |
bMWCNT–cpoly(PVC)/GCE | DPASV | 1.0–300 | 1.0–200 | 0.2 | 0.4 | 420 | 33 |
Nafion–dG–eHgFE/GCE | SWASV | 1–7 | 1–7 | 0.08 | 0.07 | 120 | 34 |
Bi–fD24C8–Nafion/gSPCE | SWASV | 0.5–60 | 0.5–60 | 0.27 | 0.11 | 180 | 35 |
MWCNTs–Nafion–Bi/hSPE | DPASV | 0.5–80 | 0.05–100 | 0.1 | 0.07 | 120 | 36 |
iERGO–jTH/kMES/GCE | SWASV | 1–40 | 1–40 | 0.1 | 0.05 | 300 | 37 |
Bi–Nafion–lDMcT–mPANI–MWCNT/GCE | DPASV | 0.02–20 | 0.1–30 | 0.01 | 0.04 | 360 | 38 |
nBiOCl–MWCNT/GCE | SWASV | 5–10 | 5–10 | 0.57 | 1.2 | 120 | 39 |
Nafion–oPDMcT–MWCNTs/GCE | DPASV | 0.05–20 | 0.1–22 | 0.03 | 0.05 | 120 | 40 |
NMC–Nafion–Bi/GCE | DPASV | 4–130 | 4–130 | 0.3 | 0.4 | 420 | Our work |
Fig. 5 Interferences caused by other cations on the stripping peak current of 50 μg L−1 Cd(II) (red) and 50 μg L−1 Pb(II) (blue) under the optimized conditions. |
Reproducibility of the proposed electrode was carefully examined by using five NMC–Nafion–Bi/GCE for simultaneous detection of 50 μg L−1 Cd(II) and 50 μg L−1 Pb(II). The RSD between electrodes was 3.3% for Cd(II) and 5.4% for Pb(II), respectively.
After storage at 4 °C for one day and half a month, the stripping signal stability of NMC–Nafion–Bi/GCE was evaluated in 50 μg L−1 Cd(II) and 50 μg L−1 Pb(II) by comparing the striping peak current between the 1st and 15th day. As illustrated in Fig. 6, the DPASV responses of Cd(II) and Pb(II) obtained at different storage time only slightly change, implying the good long-time stability of the proposed sensor.
Fig. 6 Interferences caused by storage time on the DPASV responses of 50 μg L−1 Cd(II) (red) and 50 μg L−1 Pb(II) (blue) under the optimized conditions. |
Added (μg L−1) | Found (μg L−1) | Recovery (%) | Found by ICP-MS (μg L−1) | |||
---|---|---|---|---|---|---|
Cd | Pb | Cd | Pb | Cd | Pb | |
0 | — | — | — | — | — | — |
6 | 6.5 ± 0.1 | 6.5 ± 0.1 | 108 | 108 | 6.0 | 5.8 |
8 | 7.7 ± 0.1 | 8.6 ± 0.1 | 96 | 108 | 7.9 | 8.1 |
30 | 28.6 ± 0.4 | 30.3 ± 0.4 | 95 | 101 | 29.7 | 29.9 |
Footnote |
† This authors contributed equally to the work. |
This journal is © The Royal Society of Chemistry 2017 |