Abstract
In the present study, thiol β-cyclodextrin (SH-CD) and ethylenediamine β-cyclodextrin (NH2-β-CD) were simultaneously grafted on the same interface of an Au NP deposited carboxyl SiC (Au@CSiC) nanocomposite. An electrochemical sensor for the simultaneous determination of nitrophenol isomers (o-nitrophenol, o-NP; p-nitrophenol, p-NP) using SH-CD and NH2-β-CD functionalized Au@SiC (Au@CSiC-SH/NH2-CD) nanocomposite was successfully constructed. Differential pulse voltammetry was used to quantify o-NP and p-NP within the concentration range of 0.01–150 μM under the optimal conditions. The detection limit (S/N = 3) of the sensor was 0.019 and 0.023 μM for o-NP and p-NP, respectively, indicating a low detection limit. Interference study results demonstrated that the sensor was not affected in the presence of similar aromatic compounds during the determination of NP isomers, showing high selectivity. The proposed electrochemical sensing platform was successfully used to determine NP isomers in tap water. The low detection limit and high selectivity of the proposed electrochemical sensor were caused by the high surface area, the excellent conductivity, and the more recognized (enriched) NP isomer molecules by SH-β-CD and NH2-β-CD of the Au@CSiC-SH/NH2-CD nanocomposite.
An illustration of simultaneous electrochemical determination of nitrophenol isomers using β-cyclodextrin derivative-functionalized silicon carbide.
1. Introduction
Nitrophenol (NP) is a nitroaromatic compound with three isomers, o-nitrophenol (o-NP), m-nitrophenol (m-NP) and p-nitrophenol (p-NP), and is widely used as intermediates in the chemical industry, especially in the manufacture of paints, pesticides, explosives, medicines, and plasticizers.1,2 On the other hand, some isomers of NP can be found in wastewater and agricultural run-off due to biodegradation of some organophosphorus pesticides.3 NPs are widely distributed not only in industrial wastewater and soil but also in freshwater and marine environments.4,5 It is well-known that the isomers of nitrophenol are serious environmental pollutants due to their potential toxicity (carcinogen, teratogenic and mutagenic) to human beings, animals, and plants even at a very low concentration.6–8 The harmful effects of NP on humans include headache, fever, breathing trouble, and even death at high levels of exposure.9 In addition, the NPs are readily accumulated in organisms and are hard to naturally degrade because of the high structure stability.10,11 Therefore, NP has been listed as a priority pollutant by the United States Environmental Protection Agency (USEPA).12,13 However, the toxicity of nitrophenol isomers is different; o-NP and p-NP are highly toxic and exhibit much more serious impact on the growth and metabolic activities of the organism.14,15 The permissible limit of NP in the environment has been given. For example, the permissible limit of p-NP in the environment by different agents like United States EPA and the European Commission are 0.43 μM and 0.72 nM, respectively.16 Accordingly, it is highly desirable to develop a selective and sensitive analytical method for nitrophenol isomers for environmental monitoring and diagnostic research.
β-Cyclodextrin (β-CD) is a kind of oligosaccharide composed of seven glucose units, which has a toroidal shape with a hydrophobic inner cavity and a hydrophilic exterior.16 The hydrophobic inner cavity could enable β-CD molecules to bind selectively various organic, inorganic, and biological guest molecules in their cavities to form host–guest inclusion complexes. This supramolecular inclusion complexes has been proven to show high molecular recognition and enrichment capability. Furthermore, the exterior hydrophilicity could make β-CD easily to be used as functional molecules to improve the dispersibility (solubility) of functional materials. Meanwhile, β-CD is environmentally friendly and low-cost.17 Based on these interesting characteristics, β-CD has been widely used in field of electrochemical sensing.18–22 However, in most cases, β-CD was loaded on the material surface at one interface in only one way.17 It is desired that more β-CD molecules are linked with material through different binding sites at the same interface.
It is well-known that carbon materials are widely utilized in electrochemical sensor. Generally, carbon-based materials usually have higher background currents, which is a serious disadvantage, especially in electrochemical sensing or biosensing detection system. Alternatively, noncarbon materials commonly have lower background currents.23 As one of the most valuable noncarbon materials, silicon carbide (SiC) has been considered to be a promising metal nanoparticles (NPs) support material due to its high-temperature stability, hardness, as well as chemical inertness.24 This provide a hint that SiC could be an ideal substrate for further modification of function group or anchoring noble metal NPs for high-performance electrocatalytic or electrochemical devices.
To load more β-CD molecules with material and thus improve the enrichment capacity and electrochemical detection limit of guest molecule, in the present study, thiol-β-cyclodextrin (SH-β-CD) and mono-(6-ethanediamine-6-deoxy)-β-cyclodextrin (NH2-β-CD) were grafted with silicon carbide (SiC) by Au–S bond and amido bond, respectively. Then, an electrochemical sensor based on the β-CD/SiC composite modified glassy carbon electrode (GCE) was fabricated for sensitive detection of nitrophenol isomers. The proposed electrochemical sensing platform was used to recognize guest molecules (NP isomers) as illustrated in Scheme 1.
2. Materials and methods
The experimental details are provided in ESI.†
3. Results and discussion
3.1. Characterization of the Au@CSiC and Au@CSiC-SH/NH2-CD materials
The morphologies and microstructures of the Au@CSiC were investigated using a TEM. Fig. 1A–C shows the TEM images of the Au@CSiC at different magnifications. SiC NPs demonstrated large amounts of particles approximately 20 nm. The Au NPs as spherical particles with a uniform size of ∼5 nm were fairly well monodispersed on the surface of SiC. Compared with Fig. 1A, B and C, shows that the surface of SiC was covered a layer of amorphous carbon with a thickness of ∼15 nm after a hydrothermal reaction in glucose aqueous solution, forming a clear core–shell structure. These results indicated the Au@CSiC nanocomposite was successfully prepared. Au@CSiC-SH/NH2-CD nanohybrids also were further characterized by FTIR and TGA. Fig. 1D shows the FTIR spectra of SiC, CSiC, and Au@CSiC-SH/NH2-CD respectively. The FTIR spectrum of SiC exhibited typical C–Si stretching vibrations at 824 cm−1. The strong peaks at 3435 and 1630 cm−1 were ascribed to stretching vibrations and bending vibrations of O–H in water adsorbed by SiC samples, respectively. In the case of CSiC, the weak peak at 1728 cm−1 corresponds to the C O stretching vibrations, which indicates the successful functionalization of the SiC with carboxyl groups. It is noted that the FTIR spectrum of Au@CSiC-SH/NH2-CD exhibits typical β-CD absorption features of the ring vibrations at 654 and 749 cm−1, the coupled C–O–C stretching/O–H bending vibrations at 1030 cm−1 and 1090 cm−1, –CH2 stretching vibrations at 2925 cm−1, and O–H stretching vibrations at 3435 cm−1. In addition, peaks at 1650 cm−1 may be attributed to the C O of amide groups. The results suggested that the β-CD molecules were successfully attached to CSiC.17,21 The thermal stability of SiC, CSiC, and Au@CSiC-SH/NH2-CD was investigated by TGA. As shown in Fig. 1E, for the pristine SiC, there is almost no weight loss in the measured temperature range of 35–800 °C. In the case of CSiC, an obvious mass loss can be seen at 400–700 °C, which is due to the decomposition of the surface carboxyl groups on SiC. A 4.48 wt% loss was observed when the temperature was approximately 600 °C. The Au@CSiC-SH/NH2-CD exhibited an abrupt mass loss when the temperature increased to approximately 200 °C because of the decomposition of SH-β-CD and NH2-β-CD; the mass loss reached approximately 9.92 wt% when the temperature was 600 °C, indicating that SH-β-CD and NH2-β-CD were successfully linked to the CSiC.
3.2. Electrochemical behaviors of NP isomers using the modified electrodes
EIS was performed at the potential of 0.1 V and the frequency ranges was from 101 to 105 Hz, using 2.0 mM [Fe(CN)6]3−/4− redox couple (1 : 1) with 0.1 M KCl as supporting electrolyte. The value of the electron-transfer resistance (Rct) of the modified electrode was estimated by the semicircle diameter. Fig. 1F illustrates the EIS of the bare GCE (a), CSiC/GCE (b), Au@CSiC/GCE (c), Au@CSiC-SHCD/GCE (d) and Au@CSiC-SH/NH2-CD/GCE (e). Obviously, the bare GCE exhibited a semicircle portion and the value of Rct was estimated to be approximately 850 Ω. When CSiC was loaded on the bare GCE, the Rct value of the GCE decreased to 750 Ω, indicating that CSiC had good conductivity and improved obviously the diffusion of ferricyanide toward the electrode interface.25 When the Au@CSiC was modified on the bare GCE, the Rct value decreased comparing with that of CSiC, revealing that Au NPs with excellent conductivity can facilitate the electron transfer. For the Au@CSiC-SHCD/GCE and Au@CSiC-SH/NH2-CD/GCE, their semicircles both increased to approximately 1100 and 1300 Ω. This is because of the SH-CD or NH2-CD molecule hindered the electron transfer and made the interfacial charge transfer difficult. These results further suggested that two β-CD derivatives have been successfully attached to the SiC, which were agree well with the results of IR and TGA.
The electrochemical responses of o-NP and p-NP at different modified electrodes were investigated using CVs. The CVs for the oxidation of 1.0 mM o-NP and p-NP at bare GCE (a), CSiC/GCE (b), Au@CSiC/GCE (c), Au–CSiC-SHCD/GCE (d), Au@CSiC-SH/NH2-CD/GC (e) were carried out in 0.1 M PBS (pH 6.0). As shown in Fig. 2A and B, only a well-defined reduction peak is observed during the sweep from −1.2 V to −0.2 V at all the electrodes, and no corresponding oxidation peaks are observed, indicating that the electrode response of o-NP and p-NP is a typical irreversible electrode reaction.16 The o-NP and p-NP exhibit a clear cathodic peak at approximately −0.72 and −0.83 V, respectively, which are associated with the irreversible reduction process of nitryl in aqueous solution.28,30 Furthermore, enhanced reduction currents of o-NP and p-NP using the CSiC/GCE were observed in comparison with those in the bare GCE. Meanwhile, the peak potential of o-NP and p-NP in CSiC/GCE exhibited slight negative shift (∼30 mV) than GCE. These results may be caused by good catalytic activity of CSiC.24 After the homogeneous Au NPs were monodispersed on the CSiC surface, the reduction currents of o-NP and p-NP further increased compared with CSiC, which could be ascribed to the fact that Au NPs with remarkable conductivity and large surface area could amplify the electrochemical signal. On the other hand, the reduction peak current of o-NP and p-NP at Au@CSiC-SHCD/GCE is larger than that at Au@CSiC/GCE, suggesting that β-CD molecule has good recognition capability and thus cause the excellent enrichment capacity of o-NP and p-NP. Interestingly, the reduction peak current of the NP isomers at Au@CSiC-SH/NH2-CD/GCE further increased markedly compared with that at Au@CSiC-SHCD/GCE, indicated that dual β-CD derivatives were functionalized at the same electrode interface and successfully used to improve the current signal of the NP isomers.
The DPVs for the reduction of a mixture containing 1 mM of o-NP and p-NP at bare GCE (a), CSiC/GCE (b), Au@CSiC/GCE (c), Au@CSiC-SH-CD/GCE (d) and Au@CSiC-SH/NH2-CD/GCE (e) were performed in 0.1 M PBS (pH 6.0). As shown in Fig. 2C, the current amplification and potential movement direction are similar to the CV diagram. The two well-defined peaks at −0.70 and −0.85 V correspond to o-NP and p-NP, respectively;30 these peaks are well separated and show a potential difference of 150 mV, which is an adequately large window for simultaneously determining the concentrations of mixed solutions of o-NP and p-NP. The reduction peak currents of o-NP and p-NP at the modified electrodes increased in sequence, indicating that the Au@CSiC-SH/NH2-CD/GCE is suitable for the electrochemical sensing of o-NP and p-NP. Although the β-CD macrocyclic host is non-conducting and unfavorable for the electron transfer, the reduction current of o-NP and p-NP also enhanced obviously. It is worthy to note that β-CD molecule has a hydrophobic inner cavity and a hydrophilic exterior. Nitrophenol could enter the hydrophobic inner cavity of β-CD and form a stable host–guest inclusion with o-NP and p-NP through supramolecular recognition interactions. Hence, large amount of guest molecules were enriched on the surface of the modified electrode, leading to the significant enhancement of the reduction peak current of o-NP or p-NP. Meanwhile, hydrophilic exterior of β-CD molecule could make β-CD modified CSiC into a composite with good dispersibility in aqueous solution. Such strategy of loading different supramolecular host derivatives to material and therefore enhances the molecular enrichment capability is also expected to be used in sensors for sensitive electrochemical determination of other analytes.
3.3. Optimization of experimental conditions
The pH value of the detection medium could affect the rate of mass transport to the electrode surface, especially when the redox process involves several protons.15 The effect of pH on the current response of the Au@CSiC-SH/NH2-CD toward 1 mM NP was investigated within the pH range of 4.0–8.0. Fig. 2D shows that the reduction peak current gradually increases with the increased pH from 4.0 to 6.0, which was attributed to the high concentration of protons in the solution.30 These protons replaced the molecules of nitrophenol isomers that were present on the adsorption sites on the Au@CSiC-SH/NH2-CD/GCE surface. However, further increase in pH caused a decrease in the reduction peak current because of the nitro anions that prevented the access of phenol compounds to the adsorption sites on the Au@CSiC-SH/NH2-CD/GCE surface. Therefore, pH 6.0 was selected as the optimal solution pH for the simultaneous determination of o-NP and p-NP. On the other hand, it is a general rule that a conjugate base is oxidized at less positive potentials than the corresponding acid form. A conjugate base is always more easily oxidized than the corresponding acid form, the anodic current accompanied by an antecedent acid–base equilibrium therefore always increases with increasing pH values. The observed decrease of the cathode current with increasing pH thus cannot be attributed to an acid–base reaction occurring before the electron uptake. In this study, the optimal pH of 6.0 was is considered to be the result of the synergistic effect of the above as-mentioned two reasons.
The accumulation step is a simple and effective strategy to enhance sensitivity. Thus, the effects of accumulation time and potential on the Au@CSiC-SH/NH2-CD/GCE sensor were investigated. The effect of accumulation potential on the reduction peak currents of NP isomers was also investigated. Fig. 3A shows that reduction peak currents gradually increase with increasing accumulation times of up to 150 s and then level off thereafter, which indicates that accumulation of o-NP and p-NP on the Au@CSiC-SH/NH2-CD/GCE can rapidly reach saturation. Fig. 3B shows that the highest reduction peak current is achieved at 0 V. The reduction peak currents of o-NP and p-NP were compared at different accumulation time. Accordingly, in the present study, the accumulation step was performed at 0 V for 150 s.
The effect of scan rate on the reduction of o-NP and p-NP was investigated. Fig. 4A and B show the CVs of 1 mM o-NP and p-NP on Au@CSiC-SH/NH2-CD/GCE for different scan rates. The reduction peak current of NP isomers increases gradually with an increase of scan rate. The reduction peak current increases linearly with the square root of scan rate in the range of 20 to 250 mV s−1, and the equation can be expressed as Io-NP (μA) = 6.201ν1/2 (mV s−1)1/2 + 16.617 (R2 = 0.9941) and Ip-NP (μA) = 6.215ν1/2 (mV s−1) + 17.634 (R2 = 0.9942), indicating that the reduction of o-NP and p-NP at Au@CSiC-SH/NH2-CD/GCE may be a diffusion-controlled process.28 Usually, low scan rate results in a small peak current and but a long measuring time. Although high scan rate results in a large peak current, the background of peak current also increases, which affected the stability of electrochemical sensor. Therefore, 100 mV s−1 is selected as the optimal scan rate for the determination of o-NP and p-NP. In this work, β-CD molecule was used as a factor to recognize and enrich more guest molecule (NP isomers) and thus improve the current signal of NP. Usually, β-CD molecule recognizes the most guest molecules by taking some time to reach an equilibrium state. In this study, a host-guest complex of β-CD and NP was formed and the load transfer of electrons proceeds cannot be governed by pure diffusion process. In view of the enrichment of NP by β-CD, the electrochemical reaction may be a process of mixed controls of diffusion and adsorption.
3.4. Simultaneous electrochemical determination of o-NP and p-NP using DPV
DPV was used to simultaneously quantify the o-NP and p-NP under the optimal conditions. Fig. 5A shows the DPV curves of o-NP and p-NP on the Au@CSiC-SH/NH2-CD/GCE at different concentrations. The reduction peak current increased with the increased concentration of o-NP and p-NP. The reduction currents were proportional to the o-NP concentrations in the range of 0.01–5.00 and 5.00–150.00 μM, respectively, with a detection limit of 0.019 μM (S/N = 3). The corresponding regression equations were calculated as Io-NP (μA) = 0.96Co-NP (μM) + 3.17 and Io-NP (μA) = 0.075Co-NP (μM) + 7.79 (Fig. 5B). Fig. 5C shows the corresponding calibration curve for p-NP. The reduction currents were also proportional to the concentration of p-NP in the range of 0.01–5.00 and 5.00–150.0 μM, respectively, with a detection limit of 0.023 μM (S/N = 3). The corresponding regression equations were calculated as Ip-NP (μA) = 0.81Cp-NP (μM) + 2.59 and Ip-NP (μA) = 0.076Cp-NP (μM) + 6.58, respectively. The performance of the proposed Au@CSiC-SH/NH2-CD modified electrode was compared with those of other reported electrodes.
3.5. Molecular docking
To gain an insight into the binding modes of host–guest, molecular docking was performed to study the β-CD/o-NP and β-CD/p-NP inclusion complexes. The binding modes of β-CD/o-NP and β-CD/p-NP were simulated using the DOCK6 program and shown in Fig. 6. The docking scores and binding free energy of β-CD/o-NP and β-CD/p-NP were also obtained and provided in Tables 1 and 2, respectively. Generally, if the binding energy is more negative, the interaction between the host and guest will be stronger. The results showed that the molecular docking and energy optimization conformations of β-CD/o-NP were similar before and after optimization, suggesting a signal binding mode. The guest molecule was embedded in the cavity of β-CD and the nitro group of o-NP faced to the big ring of host (Table 1), where hydrophobic interaction may play an important role in the stabilization of the host–guest inclusion complex. As shown in Table 2, the ΔGvdw (−20.5390 kcal mol−1) was much higher than ΔGele (−2.5308 kcal mol−1) in the β-CD/o-NP host–guest inclusion, indicated that hydrophobic interaction made the more contribution than electrostatic force for the formation of the host–guest inclusion complex. Also, there were obvious positive polar solvation interaction contribution (7.6752 kcal mol−1) and negative nonpolar solvation (−2.1990 kcal mol−1) contribution in β-CD/o-NP complex, indicated that the hydrophobic interaction was favorable to the host–guest binding each other. Thus, the hydrophobic interaction was considered to be the major contribution for the formation of the β-CD/o-NP inclusion complex. In the case of β-CD/p-NP complex, the similar binding interaction (hydrophobic interaction) was found to be contributed to the formation of the host–guest inclusion complex. However, the binding interaction β-CD/o-NP complex was slightly stronger than that of β-CD/p-NP complex. Unlike the case of β-CD/o-NP complex, the nitro group of p-NP faced to small ring of β-CD. The binding orientation of o-NP to β-CD was different from that p-NP to β-CD, which is considered to be the reason that caused the different binding interactions between o-NP/p-NP and β-CD. Overall, o-NP and p-NP molecules entered into cavity of β-CD molecule and formed a stable host–guest complex. Although a “stable” host–guest inclusion complex formed, which is considered to be a dynamic equilibrium process between β-CD and NP molecules.21 In this sense, NO2 group of NP molecule could reach the surface of the electrode.
Molecular docking scores of β-CD/o-NP and β-CD/p-NP complexesa.
Host | Guest | Pose | Grid score (kcal mol−1) | Grid_vdw (kcal mol−1) | Grid_es (kcal mol−1) | Int_en (kcal mol−1) |
---|---|---|---|---|---|---|
β-CD | o-NP | 1 | −24.156046 | −24.320509 | 0.164463 | 6.993269 |
2 | −23.904770 | −23.849386 | −0.055384 | 6.993267 | ||
3 | −23.850988 | −23.947292 | 0.096304 | 6.993220 | ||
p-NP | 1 | −24.025131 | −24.003979 | −0.021152 | 0.029970 |
vdw: van der Waals force; es: electrostatic force; Int_en: intramolecular energy.
Binding free energy of β-CD/o-NP and β-CD/p-NP complexesa.
Host | Guest | Pose | ΔGvdw (kcal mol−1) | ΔGele (kcal mol−1) | ΔGpol (kcal mol−1) | ΔGapol (kcal mol−1) | ΔGbind (kcal mol−1) |
---|---|---|---|---|---|---|---|
β-CD | o-NP | 1 | −20.5390 | −2.5308 | 7.6752 | −2.1990 | −17.5936 |
2 | −18.9611 | −3.8562 | 8.5227 | −2.2438 | −16.5384 | ||
3 | −20.7589 | −0.7602 | 6.5749 | −2.1896 | −17.1338 | ||
p-NP | 1 | −19.9659 | −2.0028 | 7.7360 | −2.3458 | −16.5785 |
ΔGvdw: van der Waals contribution; ΔGele: electrostatic contribution; ΔGpol: polar solvation contribution; ΔGapol: nonpolar solvation contribution; ΔGbind: binding free energy; ΔGbind = ΔGvdw + ΔGele + ΔGpol + ΔGapol.
3.6. Selectivity, reproducibility, and stability
To testify the selectivity of the proposed electrochemical sensor, the reduction currents of 10 μM o-NP and p-NP on the Au@CSiC-SH/NH2-CD/GCE were compared with signals obtained in the absence and presence of 20-fold concentrations of the interfering species (phenol, paracetamol, catechol, hydroquinone, 2,4-dinitrophenol, glucose, and citric acid). The results that the presence of the above mentioned common interferents in the system did not affect the reduction currents responses of o-NP and p-NP (Fig. 5D). In addition, no significant interference from some common ions (e.g. Ca2+, Mg2+, Zn2+, Al3+, Fe3+, SO42− and NO3−) was observed even with 500-fold excess of concentrations of NP isomers. The high selectivity of this method would be beneficial for the detection of o-NP and p-NP in actual water sample.
The reduction peak currents of 1 mM of o-NP and p-NP were measured by 6 equal Au@CSiC-SH/NH2-CD/GCE in 0.1 M PBS (pH 6.0) in parallel, and then were compared to evaluate the fabrication reproducibility of the Au@CSiC-SH/NH2-CD modified electrode. The 6 as-modified electrodes exhibited similar electrochemical responses that the relative standard deviation (RSD) of the current response values were 3.5% and 2.9% for o-NP and p-NP (data not shown), respectively, indicating satisfactory reproducibility.
Successive cyclic potential scans for 50 cycles and long-term storage assays were used to examine the stability of the Au@CSiC-SH/NH2-CD modified electrode. The as-constructed sensor show 97.5% and 96.8% of the initial peak current of 1 mM o-NP and p-NP, respectively, after 30 continuous cycle scans. Additionally, a long-term stability experiment was performed intermittently (every 5 d). The constructed sensor was stored in a refrigerator at 4 °C until use. A 97.5% of initial current responses was remained after storage for 7 d, revealing an acceptable stability of the Au@CSiC-SH/NH2-CD modified electrode.
Table 4 shows that the Au@CSiC-SH/NH2-CD/GCE exhibits a lower detection limit and a wider linear range of NP isomers than the other electrodes. Thus, the fabricated electrode could be used to simultaneously detect o-NP and p-NP in aqueous solutions with high sensitivity. The excellent detection performance of the sensor may be attributed to the following reasons: (1) the higher supramolecular recognition and enrichment capability of β-CD host molecules (SH-β-CD and NH2-CD) of the Au@CSiC-SH/NH2-CD nanocomposite; (2) the high surface area, the excellent conductivity, the excellent catalytic activity of CSiC for NP isomers reduction; (3) the outstanding conductivity properties of fairly well loaded Au NPs.
Comparison of the proposed electrochemical sensor for detection of o-NP and p-NP with others.
Sample | Electrode | Method | Linear range (μM) | LOD (μM) | Ref. |
---|---|---|---|---|---|
o-NP | Gr–Chit/ABPE | LSV | 0.4–80 | 0.20 | 26 |
MWNTs/GCE | LSV | 4–200 | 0.5 | 27 | |
CD–RGO/GCE | DPV | 7.2–64.7 | 0.14 | 11 | |
Fe3O4–Pt/GCE | DPV | 0.1–1.5 | 0.069 | 28 | |
CD–SBA/CPE | DPV | 0.2–1.4 | 0.01 | 22 | |
OMCs/GCE | DPV | 0.5–90 | 0.08 | 29 | |
Dual β-CD-SiC/GCE | DPV | 0.01–150 | 0.019 | This work | |
p-NP | S–CHIT/ABPE | LSV | 0.08–2 | 0.03 | 30 |
GO/GCE | LSV | 0.1–120 | 0.02 | 1 | |
nAg–chitosan/GCE | SWV | 0.07–2 | 0.07 | 31 | |
OMCs/GCE | DPV | 2–90 | 0.1 | 29 | |
Nano-gold/GCE | DPV | 10–1000 | 8 | 32 | |
Bridged-β-CD-MWCNT/GCE | DPV | 0.1–200 | 0.048 | 33 | |
Dual β-CD-SiC/GCE | DPV | 0.01–150 | 0.023 | This work |
3.7. Real sample analysis
The proposed method was used to detect o-NP and p-NP in tap-water and wastewater samples using standard addition methods to evaluate the feasibility of the Au@CSiC-SH/NH2-CD/GCE for real sample analysis. The results showed recoveries ranging from 98.0% to 102% with RSDs ranging from 2.5% to 3.2% (Table 3), suggested that the constructed chemical sensor based on Au@CSiC-SH/NH2-CD nanocomposite has the practical application. These results suggested that Au@CSiC-SH/NH2-CD nanocomposite modified electrode may be a better choice for the electrochemical sensing of o-NP and p-NP.
Determination of o-NP and p-NP in tap-water (n = 3).
Sample | Added (μM) | Founded (μM) | RSD (%) | Recovery (%) | ||||
---|---|---|---|---|---|---|---|---|
o-NP | p-NP | o-NP | p-NP | o-NP | p-NP | o-NP | p-NP | |
1 | 1 | 1 | 0.98 | 1.02 | 2.8 | 3.0 | 98.0 | 102.0 |
2 | 5 | 5 | 5.05 | 4.98 | 3.1 | 2.5 | 101.0 | 99.6 |
3 | 10 | 10 | 10.08 | 10.12 | 2.7 | 3.2 | 100.8 | 101.2 |
4. Conclusions
In summary, in this work, SH-β-CD and NH2-CD were simultaneously connected to Au@CSiC by Au–S bond and amide bond to prepare composite modified electrode. The electrochemical sensor was successfully used for simultaneous detection of o-NP and p-NP by DPV upon optimal experimental conditions. Due to the good electron transfer property of CSiC and the excellent molecular recognition capability of SH-β-CD and NH2-CD, the developed Au@CSiC-SHCD/NH2-CD/GCE displays excellent analytical performance for the electrochemical sensing of o-NP and p-NP: the linear range of o-NP was between 0.01–5.00 and 5–150 μM, the detection limit was 0.019 μM (S/N = 3), and the linear range of p-NP was in the range of 0.01–5.00 and 5–150 μM, the detection limit is 0.023 μM (S/N = 3). The experimental results show that the sensor has good reproducibility, stability and selectivity, which can be used for the actual water sample detection. The recoveries are between 98.0–102.0% and the results are satisfactory.
In addition, in this experiment we propose the introduction of two single modified β-CDs at the same interface of sensing plat, which enhances the molecular recognition ability of o-NP and p-NP and provides a promising electrochemical sensing platform for the simultaneous analysis of multianalytes at an identical interface. The experiment is simple, rapid and sensitive. The sensor is expected to be used in selective inspection environments pollutants, with a certain practical value.
Conflicts of interest
There are no conflicts to declare.
Supplementary Material
Acknowledgments
This work was financially supported by the National Natural Science Foundation of China (21764005, 21565029) and the Program for Donglu Scholars, Yunnan University.
Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra12715d
References
- Li J. Kuang D. Feng Y. Zhang F. Xu Z. Liu M. J. Hazard. Mater. 2012;201–202:250–259. doi: 10.1016/j.jhazmat.2011.11.076. [DOI] [PubMed] [Google Scholar]
- Zhang W. Chang J. Chen J. Xu F. Wang F. Jiang K. Gao Z. Res. Chem. Intermed. 2012;38:2443–2455. doi: 10.1007/s11164-012-0560-7. [DOI] [Google Scholar]
- Whitacre D. M., Reviews of environmental contamination and toxicology, Springer, New York, 2010 [PubMed] [Google Scholar]
- Thouand G. Friant P. Bois F. Cartier A. Maul A. Block J. C. Ecotoxicol. Environ. Saf. 1995;30:274–282. doi: 10.1006/eesa.1995.1031. [DOI] [PubMed] [Google Scholar]
- Thouand G. Captdevielle B. Block J. C. Ecotoxicol. Environ. Saf. 1996;33:261–267. doi: 10.1006/eesa.1996.0033. [DOI] [PubMed] [Google Scholar]
- Podeh M. R. H. Bhattacharya S. K. Qu M. Water Res. 1995;29:391–399. doi: 10.1016/0043-1354(94)00193-B. [DOI] [Google Scholar]
- Schüürmann G. Somashekar R. K. Kristen U. Environ. Toxicol. Chem. 1996;15:1702–1708. [Google Scholar]
- Saha N. C. Bhunia F. Kaviraj A. Bull. Environ. Contam. Toxicol. 1999;63:195–202. doi: 10.1007/s001289900966. [DOI] [PubMed] [Google Scholar]
- Pohanish R. P., Sittig's Handbook of toxic and hazardous chemicals and carcinogens, William Andrew, Oxford, 2008 [Google Scholar]
- Liu Z. Du J. Qiu C. Huang L. Ma H. Shen D. Ding Y. Electrochem. Commun. 2009;11:1365–1368. doi: 10.1016/j.elecom.2009.05.004. [DOI] [Google Scholar]
- Liu Z. Ma X. Zhang H. Lu W. Ma H. Hou S. Electroanalysis. 2012;24:1178–1185. doi: 10.1002/elan.201100735. [DOI] [Google Scholar]
- US Environmental Protection Agency Fed. Regist. 1989;52:131. [PubMed] [Google Scholar]
- Asadpour-Zeynali K. Najafi-Marandi P. Electroanalysis. 2011;23:2241–2247. doi: 10.1002/elan.201100103. [DOI] [Google Scholar]
- Megharaj M. Pearson H. W. Venkateswarlu K. Arch. Environ. Contam. Toxicol. 1991;21:578–584. doi: 10.1007/BF01183881. [DOI] [Google Scholar]
- Uberoi V. Bhattacharya S. K. Water Environ. Res. 1997;69:146–156. doi: 10.2175/106143097X125290. [DOI] [Google Scholar]
- Wei Y. Kong L. T. Yang R. Wang L. Liu J. H. Huang X. J. Langmuir. 2011;27:10295–10301. doi: 10.1021/la201691c. [DOI] [PubMed] [Google Scholar]
- Zhu G. Yi Y. Chen J. TrAC, Trends Anal. Chem. 2016;80:232–241. doi: 10.1016/j.trac.2016.03.022. [DOI] [Google Scholar]
- Zhao H. Yang L. Li Y. Ran X. Ye H. Zhao G. Zhang Y. Liu F. Li C. P. Biosens. Bioelectron. 2017;89:361–369. doi: 10.1016/j.bios.2016.07.016. [DOI] [PubMed] [Google Scholar]
- Zhang Z. Gu S. Ding Y. Shen M. Jiang L. Biosens. Bioelectron. 2014;57:239–244. doi: 10.1016/j.bios.2014.02.014. [DOI] [PubMed] [Google Scholar]
- Zhu G. Zhang X. Gai P. Gao P. Zhang X. Chen J. Nanoscale. 2012;4:5703–5709. doi: 10.1039/C2NR31378B. [DOI] [PubMed] [Google Scholar]
- Guo Y. Guo S. Ren J. Zhai Y. Dong S. Wang E. ACS Nano. 2010;4:4001–4010. doi: 10.1021/nn100939n. [DOI] [PubMed] [Google Scholar]
- Xu X. Liu Z. Zhang X. Duan S. Xu S. Zhou C. Electrochim. Acta. 2011;58:142–149. doi: 10.1016/j.electacta.2011.09.015. [DOI] [Google Scholar]
- Yang L. Zhao H. Fan S. Li B. Li C. P. Anal. Chim. Acta. 2014;852:28–36. doi: 10.1016/j.aca.2014.08.037. [DOI] [PubMed] [Google Scholar]
- Wu W. C. Chang H. W. Tsai Y. C. Chem. Commun. 2011;47:6458–6460. doi: 10.1039/C1CC11162K. [DOI] [PubMed] [Google Scholar]
- Oliveros A. Guiseppi-Elie A. Saddow S. E. Biomed. Microdevices. 2013;15:353–368. doi: 10.1007/s10544-013-9742-3. [DOI] [PubMed] [Google Scholar]
- Deng P. Xu Z. Li J. Microchim. Acta. 2014;181:1077–1084. doi: 10.1007/s00604-014-1206-9. [DOI] [Google Scholar]
- Luo L. Zou X. Ding Y. Wu Q. Sens. Actuators, B. 2008;135:61–65. doi: 10.1016/j.snb.2008.07.019. [DOI] [Google Scholar]
- Gerent G. G. Spinelli A. J. Hazard. Mater. 2017;330:105–115. doi: 10.1016/j.jhazmat.2017.02.002. [DOI] [PubMed] [Google Scholar]
- Zhang T. Lang Q. Yang D. Li L. Zeng L. Zheng C. Li T. Wei M. Liu A. Electrochim. Acta. 2013;106:127–134. doi: 10.1016/j.electacta.2013.05.055. [DOI] [Google Scholar]
- Deng P. Xu Z. Feng Y. Li J. Sens. Actuators, B. 2012;168:381–389. doi: 10.1016/j.snb.2012.04.041. [DOI] [Google Scholar]
- de Lima C. A. Silva P. S. D. Spinelli A. Sens. Actuators, B. 2014;196:39–45. doi: 10.1016/j.snb.2014.02.005. [DOI] [Google Scholar]
- Chu L. Han L. Zhang X. J. Appl. Electrochem. 2011;41:687–694. doi: 10.1007/s10800-011-0281-4. [DOI] [Google Scholar]
- Yang L. Fan S. Deng G. Li Y. Ran X. Zhao H. Li C. P. Biosens. Bioelectron. 2015;68:617–625. doi: 10.1016/j.bios.2015.01.059. [DOI] [PubMed] [Google Scholar]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.