Guo Zhaoab,
Hui Wangab and
Gang Liu*ab
aKey Lab of Modern Precision Agriculture System Integration Research, Ministry of Education of China, China Agricultural University, Beijing 100083, P. R. China. E-mail: pac@cau.edu.cn; 1252624780@qq.com; Fax: +86-010-62736741; Tel: +86-010-62736741
bKey Lab of Agricultural Information Acquisition Technology, Ministry of Agricultural of China, China Agricultural University, Beijing 100083, P. R. China
First published on 30th January 2018
In this study, a simple but effective electrochemical method was developed to minimize the interference from real soil samples and increase the sensitivity of Pb(II) and Cd(II) detection by square-wave anodic stripping voltammetry (SWASV) using a novel electrochemical measurement system, which can be used for the on-site determination of trace Cd(II) and Pb(II) in real soil samples. The method involved performing SWASV following double deposition and stripping steps at two in situ plated bismuth-film electrodes with drastically different surface properties. Pb(II) and Cd(II) were first deposited on an in situ plated bismuth-film graphite carbon paste electrode (Bi/GCPE). When the first deposition was finished, the GCPE was moved to a micro-electrolytic cell to perform the first stripping step. The following measurements were performed with the other deposition and stripping steps using a highly sensitive in situ plated bismuth-film multiwalled carbon nanotube–Nafion composite modified glassy carbon electrode (Bi/MWCNT–Nafion/GCE) as the working electrode. Pb(II), Cd(II) and Bi(III) stripped from the GCPE in the micro-electrolytic cell were partially deposited on the MWCNT–Nafion/GCE, and the stripping current signals were obtained from their oxidation during the second stripping step. Considering the small volume of the micro-electrolytic cell, the concentrations of Cd(II) and Pb(II) were drastically higher than those in the bulk solution, and therefore, the detection limits were reduced. Under the optimized conditions, the concentrations in the linear range spanned from 1.0 to 45.0 μg L−1 for both Pb(II) and Cd(II), with a detection limit of 0.03 μg L−1 for Pb(II) and 0.02 μg L−1 for Cd(II) (S/N = 3). Finally, analyses of real samples were performed to detect trace levels of Pb(II) and Cd(II) in soil with satisfactory results.
Over the past several decades, the development of highly effective analytical methods, such as inductively coupled plasma atomic emission spectroscopy (ICP-AES),7 atomic fluorescence spectrometry,8 atomic absorption spectrometry (AAS),7 colourimetric analysis,9 inductively coupled plasma mass spectrometry (ICP-MS)10,11 and ultraviolet-visible (UV-vis) spectrometry,12,13 for the determination of toxic heavy metals (HMs) at trace levels has attracted increasing interest. Although these methods are sensitive for the determination of HMs at trace levels, long analysis times and tedious sample preparation methods are needed to meet requirements for real sample analysis. Consequently, these techniques are not suitable for on-field analysis and emergency detection.
Electrochemical methods, which have the unique advantages of ease of use, low cost, short analysis time and high sensitivity,14,15 have gained significant interest in the detection of HMs as alternatives to spectroscopic-based detection methods. Anodic stripping voltammetry (ASV)16–18 is one of the most commonly used methods to determine different types of HMs because of the unique advantages of ASV, such as low detection limit, high sensitivity and wide linear dynamic range. Square-wave ASV (SWASV) has been widely used in the analysis of HMs at trace levels with high sensitivity and stability.19–21
However, soil samples contain many complicated interferents and complex matrices, which result in enormous gaps between real conditions and lab measurements. The presence of natural organic compounds in soil samples and the interference caused by other HMs, which have negative impacts on the stripping procedure, are the main problems associated with electrochemical methods. These drawbacks increase the electrolyte background to high levels and interfere with detection of the target HMs. To the best of our knowledge, few reports22,23 of HM detection in soil samples using ASV methods have been published in recent years. Therefore, a method with a high anti-interference ability and high sensitivity would be a significant advancement to improve the measurement performance of stripping voltammetry methods for the detection of trace levels of HMs in soil. Chemically modified electrodes (CMEs) are being actively studied to minimize interference from other metal ions, which can effectively improve the detection performances of electrodes by providing effective preconcentration, a selective reaction surface, good repeatability, and low background current over a wide potential range.24–27
For many years, carbon paste electrodes (CPEs) have experienced significant popularity for use in electrochemical analysis because of their low residual currents, low cost and renewable surfaces. The presence of monolayer and/or multilayer graphene provide graphite carbon paste electrodes (GCPEs) with numerous excellent characteristics, such as remarkable accumulation ability and dramatically large specific surface area,28 which are formed with the help of a grinding process.29 Multiwalled carbon nanotubes (MWCNTs) have been widely used as modifiers for electrodes due to their unique features, such as highly efficient catalytic activity towards certain target analytes, unique electrical conductivity and large electrochemically active surface area. Modified electrodes based on bismuth films and carbon nanotubes are excellent tools for the electrochemical analysis of trace HMs.30–33 Nafion (NA) has gained significant attention as a type of electrode modifier for HM determination due to its special characteristics, such as good HM preconcentration ability and excellent mechanical stability.34 Moreover, NA has been successfully applied to modify electrodes in combination with mercury and bismuth films.35,36
In the investigations described in this paper, a novel method is developed to simultaneously minimize the interference of other HMs on the target HMs and improve the determination sensitivity for Pb(II) and Cd(II) by SWASV. The procedure was performed with an electrochemical measurement system containing an electrochemical workstation, a micro-electrolytic cell and two combined working electrodes (i.e., Bi/GCPE and Bi/MWCNT–Nafion/glassy carbon electrode (Bi/MWCNT–Nafion/GCE); Bi/GCPE = in situ plated bismuth-film GCPE and Bi/MWCNT–Nafion/GCE = in situ plated bismuth-film MWCNT–Nafion/GCE), which possessed significantly different surface area properties. Under optimized conditions, the application of ASV and the electrochemical measurement system following the simultaneous deposition and stripping using two different combined electrodes in one measurement contributed to a decrease in the detection limits of Cd(II) and Pb(II) due to concentrating effects. Moreover, the interference of other HMs on the determination of Pb(II) and Cd(II) by SWASV was effectively improved by skillfully transferring the location of the detection of HMs by SWASV from soil extracts to acetate buffer solutions, which supplied a detection environment without interference from other HMs. Finally, the analysis of Cd(II) and Pb(II) in soil samples was performed to validate the feasibility and practicality of this method.
The MWCNT–Nafion/GCE composite was prepared according to the following procedure. The GCE surface was polished by 0.05 mm alumina powder and then rinsed with HNO3–H2O (1:1 by volume), absolute ethanol, and water. The MWCNT dispersion was prepared by adding 1 mg of MWCNTs into 4 mL of a dimethyl formamide (DMF) solution to obtain a 0.25 mg mL−1 black suspension with the help of ultrasonic agitation for 2.5 h. Then, 500 μL of 1 wt% Nafion was added to the MWCNT dispersion to form a composite solution of MWCNT–Nafion. Next, a 6 μL suspension of the MWCNT–Nafion composite was coated onto the GCE surface and solidified by irradiating for 10 min using an infrared lamp to obtain the MWCNT–Nafion/GCE.
As shown in Fig. S1 ESI,† the height and diameter of the stirring chamber were 48 mm and 22 mm, respectively, which were determined by the height of the composite electrode and the overall size of the system. The body of the composite electrode was made of PTFE and had a height of 10 mm. The volume of acetate buffer solution added to the stirring chamber during the second deposition and stripping step greatly influences the detection performance of this method. On the one hand, if the volume is too large, it would reduce the concentration performance of HMs, and then reduce the detection sensitivity. On the other hand, if the volume is too small, a vortex would be formed in the stirring chamber, which would affect the detection results. In addition, the volume of acetate buffer solution added to the stirring chamber is also determined by the size of the three-electrode system. Considering the above situation, 1 mL of acetate buffer solution (0.1 M, pH 5.0) was added to the stirring chamber for the second deposition and stripping step.
Fig. 1 Schematic illustration of the sensitive determination of Cd(II) and Pb(II) using the double deposition and stripping steps with an electrochemical measurement system. |
The first combined electrode was disconnected from the electrochemical workstation, and then, the electrochemical workstation was connected to the second combined electrode. The second deposition step was performed at the second combined electrode (i.e., Bi/MWCNT–Nafion/GCE) at a potential of −1.2 V for 280 s. Then, following the second stripping step at a frequency of 25 Hz, a square-wave voltammogram was recorded as the potential was changed from −1.2 to +0.2 V without stirring. The frequency, step amplitude and pulse amplitude were 25 Hz, 5 mV and 25 mV, respectively. During the stripping step, most of heavy metals would strip from the surface of the electrode, but maybe a small amount of HMs still on the electrode surface, which would be effect the next detection. Moreover, the stripping potential (oxidation potential) of cadmium, lead and bismuth were ∼−0.8 V, ∼−0.57 V and ∼−0.15 V. In order to remove the residual HMs and Bi film from the GCE surface, a more positive potential +0.31 V using potentiostatic method was performed on the second combined electrode for 120 s to remove the residual bismuth film and metals on the surface of the MWCNT–Nafion/GCE after the second stripping step.
The surface area of the GCPE played a key role in the determination of HMs using the developed method, by influencing the preconcentration of the HMs, such as Pb(II) and Cd(II), on the electrode. Therefore, SEM was performed to characterize the surface morphology of the GCPE. The SEM images of the GCPE at two different magnifications are shown in Fig. 3A and B, displaying a multilayer structure of graphite flakes with clearly visible layers, which may supply more deposition sites for HMs and then improve the preconcentration efficiency of the HMs on the surface of the electrode. This observation is highly consistent with the above experimental results shown in Fig. 2. Moreover, EDS mapping acquired across representative areas of the corresponding GCPE with the deposition of Pb(II) and Cd(II) reveals that a large amount of Pb(II) and Cd(II) was electrodeposited on the electrode surface, as shown in Fig. 3C and D, likely in the form of intermetallic compounds. However, the multilayer structure of graphite flakes may reduce the conductivity of the electrode surface. In addition, because of the large surface area and adsorption property of GCPE, a large number of HMs deposited on the electrode surface may hard to strip from the surface of the electrode easily, which would reduce the rapid oxidation efficiency of HMs.
Fig. 3 (A and B) SEM images of the GCPE at two different magnifications. (C and D) EDS mappings of the GCPE. |
The stripping voltammetry behaviours of Cd(II) and Pb(II) on the bismuth-film-modified GCE were characterized by a CHI660D electrochemical workstation. The bismuth film was in situ modified19,22 with a Bi(III) concentration of 600 μg L−1. As probe metal ions, the concentrations of both Cd(II) and Pb(II) were 20 μg L−1. As shown in Fig. S2A ESI†, the stripping peak signals of Pb(II) and Cd(II) at the GCE were weak and unobvious. Comparatively, the Bi/GCE exhibited higher stripping peak signals for Cd(II) and Pb(II), suggesting that the presence of Bi could promote the reduction of Pb(II) and Cd(II) due to the unique advantages of the bismuth-film-modified electrodes, such as the ability to form alloys with the HMs. Eight repeated measurements of 20 μg L−1 Cd(II) and Pb(II) in acetate buffer solution (pH 5.0, 0.1 M) were performed to verify the reproducibility and stability of the bismuth-film-modified GCE, as shown in Fig. S2B ESI.† The results indicate that the stripping peak signals of Pb(II) and Cd(II) on the bismuth-film-modified GCE were reproducible. The relative standard deviation (RSD) of the eight repeated measurements was 2.39% and 1.68% for Pb(II) and Cd(II), respectively. Under the optimum experimental conditions, the bismuth-film-modified GCE exhibited remarkable stability and reproducibility in the stripping analysis of trace levels of Pb(II) and Cd(II), providing a reliable and stable substrate for the modification of the MWCNT–Nafion composite.
Fig. 4 shows the SWASV responses of 20 μg L−1 Pb(II) and Cd(II) at the GCE (curve a) using a general SWASV technique with single deposition and stripping steps, at the Bi/GCE using double deposition and stripping steps (curve b) (the first electrode is the Bi/GCPE, and the second electrode is the Bi/GCE) and at the Bi/MWCNT–Nafion/GCE using double deposition and stripping steps (curve c) (the first electrode is the Bi/GCPE, and the second electrode is the Bi/MWCNT–Nafion/GCE). The stripping peak signals obtained from the SWASV measurements of 20 μg L−1 Pb(II) and Cd(II) at the Bi/MWCNT–Nafion/GCE using double deposition and stripping steps were higher than those in the other two cases. These results may be because of the exceptional characteristics of the MWCNT–Nafion/GCE, such as the unique electrical conductivity, large specific surface area and the good HM preconcentration and stripping ability of the MWCNT–Nafion composite film on the surface of the electrode. The excellent preconcentration ability of the synthesized GCPE was again highlighted by these experimental results. Moreover, the reproducibility of the Bi/GCPE and Bi/MWCNT–Nafion/GCE was validated by five repeated measurements of 20 μg L−1 Cd(II) and Pb(II) with 600 μg L−1 Bi(III) in acetate buffer solution (pH 5.0, 0.1 M). The RSD of the five repeated measurements was 2.28% and 2.23% for Pb(II) and Cd(II) using the Bi/GCPE, respectively, and 2.04% and 1.95% using the Bi/MWCNT–Nafion/GCE, respectively.
The following experiments were performed to optimize the first deposition step and stripping step by setting the parameters of second deposition step and stripping step as following: pH = 5.0; deposition time = 280 s; deposition potential = −1.2 V. The parameters of the first deposition step and the stripping step were determined by the magnitude of stripping currents on the Bi/MWCNT–Nafion/GCE. As shown in Fig. 5A, double-stripping voltammetry was performed using the supporting electrolyte with different pH values for the first deposition step and stripping step. The maximum value of the stripping peak signal on the Bi/MWCNT–Nafion/GCE occurred at a pH of 5.0, and therefore, a pH of 5.0 was chosen for the first deposition step. Fig. 5B displays the influence of the Bi(III) concentration on the stripping peak signals of Pb(II) and Cd(II) without the additional addition of Bi(III) to the micro-electrolytic cell during the second deposition and stripping steps. A Bi(III) concentration of 600 μg L−1 was shown to be the optimal value to obtain the maximal values of the stripping responses of Cd(II) and Pb(II). The effect of the deposition potential on the stripping responses of Pb(II) and Cd(II) in the first deposition was investigated in the potential range of −0.8 to −1.4 V for a deposition of 700 s, as shown in Fig. 5C. The maximal stripping peak signals for both Pb(II) and Cd(II) appeared at a deposition potential of −1.2 V. Therefore, a deposition potential of −1.2 V was adopted in the first deposition step for further measurements. In the double-stripping voltammetry method based on SWASV, the deposition time plays a key role in the improvement of the HM detection sensitivity. Thus, the optimal deposition times for the first deposition step were determined by the following experiments, as shown in Fig. 5D. The deposition time for the first deposition step was varied over the range of 100–1000 s, the peak currents of the target Pb(II) and Cd(II) at the Bi/MWCNT–Nafion/GCE increased with an increase of the deposition time for the first deposition. However, when the deposition time was longer than 700 s, the increase in the peak currents levelled off. Considering both of the efficiency and sensitivity, a deposition time of 700 s was adopted for the first deposition step. Additionally, the effect of the parameters i. e., pH, deposition time, deposition potential and Bi(III) concentration, for the second deposition step and stripping step was also investigated by setting the parameters of first deposition step and fist stripping step as following: pH = 5.0; deposition time = 700 s; deposition potential = −1.2 V and Bi(III) concentration = 600 μg L−1.
Fig. 5 Effects of the (A) pH, (B) Bi(III) concentration, (C) deposition potential and (D) deposition time for the first deposition step on the stripping peak currents of 30 μg L−1 Cd(II) and Pb(II). |
According to the optimization results of the parameters for second deposition step and stripping step, a pH of 5.0, deposition time of 280 s and a deposition potential of −1.2 V were chosen for the second deposition step and stripping step. Additionally, the experimental results indicated that further addition of Bi(III) to the testing solution in the micro-electrolytic cell for the second deposition step and stripping step did not improve the peak current signals, indicating that the amount of Bi(III) stripped from the GCPE after the first stripping step was sufficient to meet requirements for detection. Therefore, the optimal Bi(III) concentration in the bulk solution was 600 μg L−1 for the first deposition step, and additional Bi(III) was not added to the testing solutions for the second deposition step.
To assess the effectiveness of the SWASV measurements following the double deposition and stripping steps, the calibration curves of Pb(II) and Cd(II) using a general SWASV technique following a single deposition and stripping step at a Bi/MWCNT–Nafion/GCE were also investigated. Under the optimized conditions, in the concentration range of 1.0 to 45 μg L−1, the calibration curve was y = 1.08x − 1.56 with a correlation coefficient of 0.991 for Cd(II) and y = 0.404x + 0.885 with a correlation coefficient of 0.998 for Pb(II). The limit of detection (S/N = 3) was 2.3 μg L−1 for Pb(II) and 1.2 μg L−1 for Cd(II).
The new method clearly shows a higher sensitivity (slope of the calibration curve) than the single-step method. The sensitivity was over 7 times higher than that obtained by the general stripping voltammetry technique, which resulted in a two orders of magnitude difference between the reported DLs. Considering the small volume of the micro-electrolytic cell, the concentrations of Cd(II) and Pb(II) were dramatically higher than those in the bulk solution, therefore reducing the detection limits.
The comparative analysis of the double-stripping voltammetry method and the general stripping voltammetry technique shows that the analytical performance of this method using double deposition and stripping steps is comparable to and even better than the general stripping voltammetry technique, which offered lower detection limits. Compared with the general stripping voltammetry technique, the developed double-stripping voltammetry method exhibited a higher sensitivity, potentially because of the preconcentration of HMs, which reduces the volume of the testing buffer solution. Moreover, the excellent electrochemical properties, such as the unique electrical conductivity, the large specific surface area and the good HM preconcentration and stripping ability, of the Bi/MWCNT–Nafion/GCE also contributed to this remarkable sensitivity.
Propagating errors will directly affect the stability and reproducibility of the developed method. The stability and reproducibility of the improved stripping voltammetry method were tested via five repeated measurements of 30 μg L−1 Pb(II) and Cd(II) in 0.1 M acetate buffer solution (pH 5.0). The stripping peak currents of Pb(II) and Cd(II) in the second stripping step after a complete testing process indirectly reflect the stability and reproducibility of the improved stripping voltammetry method. The stripping peak currents of Pb(II) and Cd(II) in the second stripping step after a complete testing process were reproducible, with RSDs of 2.24% for Cd(II) and 2.37% for Pb(II), which indicated the proposed method has a good stability and reproducibility. The proposed method was composed of two deposition and stripping steps, which a GCPE was used for the first deposition and stripping step and the MWCNT–Nafion/GCE was used for the second deposition and stripping step. The good stability and reproducibility of MWCNT–Nafion/GCE and GCPE play an important role in the stability and reproducibility of the proposed method. However, in the first deposition step, in addition to the target HMs, other HM ions in real samples may also be deposited on the surface of the electrode. The influence of various possible interferents, such as Cu(II), Na(I), As(III), Cr(II), K(I), Ca(II) and Zn(II), on the determination of Pb(II) and Cd(II) was examined under the optimized conditions. At higher concentrations of interference ions, no significant changes were observed in the stripping peak currents of either HM (changes in peak currents <10%), except in the presence of Cu(II), which negatively affected the stripping peak currents. Nevertheless, this Cu(II) interference could be reduced by the addition of 0.1 mM ferrocyanide to the sample extract solutions to form an insoluble and stable copper–ferrocyanide complex with the help of a ligand.40–43
Moreover, HMs in the double electrode layer may be lost in the transfer process of the GCPE after the first deposition step. In addition, target HMs on the electrode surface may also be oxidized during the transfer process. Therefore, after the first deposition step, the GCPE must be rapidly transferred to the micro-electrolytic cell (in no more than 2 s); however, partial oxidation is unavoidable. The results show that the stripping signals of the HMs after the second deposition step are higher than those obtained from conventional single-stripping voltammetry. This may be because the GCPE has a large specific surface area and can adsorb large amounts of HMs.28,29 Furthermore, the micro-electrolytic cell is able to concentrate the HM ions, which improved the voltammetric signal. In other words, the loss of HMs during the transfer process after the first deposition step does not affect the final detection performance. Moreover, detection of the target HMs was performed using the relationship established between the stripping voltammetry signals from the second stripping step and the HM concentrations in the samples. Interference in the transfer process does not affect the detection results. However, after the first deposition step, the GCPE transfer process is performed manually, during which the GCPE is exposed to the air. If the transfer rate is slow, the detection results will be negatively affected, which is a key issue to be addressed in our future research.
Table 1 shows a comparison of the analytical performances obtained in this work and previous works. The detection limits of Pb(II) and Cd(II) obtained by the developed method are lower than those in most previous reports. Moreover, CMEs used for HM detection were most often used in aqueous samples, while methods using CMEs for soil sample analysis are rarely reported. In addition, the strategy present in this paper consists of a deposition step on a “real” sample, followed by transfer of the electrode to a micro-electrolysis cell where the contents are stripped from the electrode, and then re-deposited on a different electrode which enhances the signal level and reduces the impact of interfering matrix effects (e.g. by using an optimized acetate buffer and optimized conditions), since it allows to preconcentrate the sample and to perform the analysis under more controlled and interference-free conditions, which effectively reduces the interference of background matrices and the pH, indicating the excellent performance of the developed method for the detection of Pb(II) and Cd(II).
Electrode | Technique | Linear range (μg L−1) | Detection limit (μg L−1) | pH effects | Interferents | Matrix effects | Applicability to specific samples | Reference | ||
---|---|---|---|---|---|---|---|---|---|---|
Cd(II) | Pb(II) | Cd(II) | Pb(II) | |||||||
GO-MWCNT/GCE | DPASV | 0.5–30 | 0.5–30 | 0.1 | 0.2 | Presence | Zn(II) and Cu(II) | Presence | Effluent | 44 |
AG-NA/GCE | DPASV | 5–100 | 5–100 | 0.07 | 0.05 | Presence | No description | Presence | Tap water | 45 |
Bi-D24C8/Nafion/SPCE | SWASV | 0.5–60 | 0.5–60 | 0.27 | 0.11 | Presence | Cu(II) | Presence | Rice | 46 |
GR/PSS/Bi/SPE | DPASV | 0.5–120 | 0.5–120 | 0.04 | 0.09 | Presence | Zn(II), Sn(II), Ni(II) and Cu(II) | Presence | Water | 47 |
ERGO–TH–MES/GCE | SWASV | 1–40 | 1–40 | 0.1 | 0.05 | Presence | No description | Presence | Water | 48 |
BiOCl/MWCNT/GCE | SWASV | 5–50 | 5–50 | 1.2 | 0.57 | Presence | Cu(II) | Presence | Pore water | 49 |
Bi-GCPE | SWASV | 0.1–50 | 0.1–50 | 0.07 | 0.04 | Presence | No description | Presence | Tap water | 50 |
Bi-xerogel/Nafion/GCE | SWASV | 0.56–11.24 | 1.04–20.72 | 0.37 | 1.3 | Presence | Cu(II) | Presence | Tap, table and lake water | 51 |
Nafion-G/GCE | DPASV | 1.5–30 | 0.5–50 | 0.02 | 0.02 | Presence | Triton X-100 | Presence | Water | 52 |
MWCNT/poly(PCV)/GCE | DPASV | 1–300 | 1–200 | 0.2 | 0.4 | Presence | Fe(III), Ag(I), Ni(II) and Cu(II) | Presence | Water | 53 |
Bi/GCPE and Bi/MWCNT-Nafion/GCE | SWASV | 1–45 | 1–45 | 0.02 | 0.03 | Not obvious | Cu(II) | Not obvious | Soil | This work |
Under the optimized conditions, in the concentration range of 1.0 to 45 μg L−1, the peak current signals of Cd(II) and Pb(II) increased linearly with increasing concentration, and the calibration curves were y = 5.57x + 9.59 with a correlation coefficient of 0.997 for Cd(II) and y = 4.54x + 5.33 with a correlation coefficient of 0.997 for Pb(II). These results showed that the performance of the developed method also depended on the supporting electrolyte due to complicated influences from the dissolved constituents in the soil, as the real samples showed lower sensitivity and selectivity than the laboratory samples. Specifically, the calibration curves obtained from the pure acetate buffer solution were not suitable for evaluation of the real samples. Thus, these calibration curves were selected for the analyses of trace Pb(II) and Cd(II) in real samples soil. Four soil samples obtained from a farm in China were used for real sample analysis by the developed double-stripping voltammetry method. Additionally, the detection results were compared with those obtained by AAS, as summarized in Table 2. The experimental results showed no significant difference between the two sets of data, indicating the good reliability of the developed method. Recovery tests were performed to verify the feasibility of the developed method. The average recovery was 98.68% for Pb(II) and 102.42% for Cd(II), respectively. The recovery tests further demonstrate that the developed method can determine trace levels of Pb(II) and Cd(II) in real samples.
Sample no. | Added (μg L−1) | Found by SWASVa (μg L−1) | Found by AASa (μg L−1) | Recovery (%) | |||
---|---|---|---|---|---|---|---|
Cd(II) | Pb(II) | Cd(II) | Pb(II) | Cd(II) | Pb(II) | ||
a Mean value ± standard deviation. | |||||||
1 | — | 3.56 ± 0.18 | 5.42 ± 0.25 | 3.68 ± 0.15 | 5.49 ± 0.18 | — | — |
2.00 | 5.74 ± 0.22 | 7.38 ± 0.16 | 109.00 | 98.00 | |||
4.00 | 7.62 ± 0.10 | 9.40 ± 0.15 | 101.50 | 99.50 | |||
2 | — | 4.32 ± 0.12 | 4.78 ± 0.21 | 4.75 ± 0.20 | 4.96 ± 0.12 | — | — |
3.00 | 7.48 ± 0.23 | 7.65 ± 0.16 | 105.33 | 95.67 | |||
6.00 | 10.53 ± 0.18 | 10.64 ± 0.24 | 103.50 | 97.67 | |||
3 | — | 5.74 ± 0.16 | 4.93 ± 0.12 | 5.93 ± 0.16 | 5.12 ± 0.14 | — | — |
4.00 | 9.85 ± 0.23 | 8.86 ± 0.26 | 102.75 | 98.25 | |||
8.00 | 13.60 ± 0.14 | 13.04 ± 0.25 | 98.25 | 101.38 | |||
4 | — | 3.60 ± 0.21 | 4.15 ± 0.13 | 3.84 ± 0.22 | 4.26 ± 0.18 | — | — |
5.00 | 8.49 ± 0.22 | 9.06 ± 0.20 | 97.80 | 98.20 | |||
10.00 | 13.72 ± 0.18 | 14.23 ± 0.25 | 101.20 | 100.80 |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra12767g |
This journal is © The Royal Society of Chemistry 2018 |