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RESEARCH PAPER Simultaneous voltammetric detection of cadmium(II), arsenic(III), and selenium(IV) using gold nanostar–modified screen-printed carbon electrodes and modified Britton-Robinson buffer Dingnan Lu1 & Connor Sullivan1 & Eric M. Brack2 & Christopher P. Drew2 & Pradeep Kurup1 Received: 19 February 2020 /Revised: 30 March 2020 /Accepted: 3 April 2020 # Springer-Verlag GmbH Germany, part of Springer Nature 2020 Abstract The present work reports a newly developed square wave anodic stripping voltammetry (SWASV) methodology using novel gold nanostar–modified screen-printed carbon electrodes (AuNS/SPCE) and modified Britton-Robinson buffer (mBRB) for simultaneous detection of trace cadmium(II), arsenic(III), and selenium(IV). During individual and simultaneous detection, Cd2+, As3+, and Se4+ exhibited well-separated SWASV peaks at approximately − 0.48, − 0.09, and 0.65 V, respectively (versus Ag/AgCl reference electrode), which enabled a highly selective detection of the three analytes. Electrochemical impedance spectrum tests showed a significant decrease in charge transfer resistance with the AuNS/SPCE (0.8 kΩ) compared with bare SPCE (2.4 kΩ). Cyclic voltammetry experiments showed a significant increase in electroactive surface area with electrode modification. The low charge transfer resistance and high electroactive surface area contributed to the high sensitivity for Cd2+ (0.0767 μA (0.225 μg L−1)−1), As3+ (0.2213 μA (μg L−1)−1), and Se4+ (μA (μg L−1)−1). The three analytes had linear stripping responses over the concentration range of 0 to 100 μg L−1, with the obtained LoD for Cd2+, As3+, and Se4+ of 1.6, 0.8, and 1.6 μg L−1, respectively. In comparison with individual detection, the simultaneous detection of As3+ and Se4+ showed peak height reductions of 40.8% and 42.7%, respectively. This result was associated with the possible formation of electrochemically inactive arsenic triselenide (As2Se3) during the preconcentration step. Surface water analysis resulted in average percent recov- eries of 109% for Cd2+, 93% for As3+, and 92% for Se4+, indicating the proposed method is accurate and reliable for the simultaneous detection of Cd2+, As3+, and Se4+ in real water samples. Keywords Metals/heavymetals . Stripping analysis . Electroanalytical methods . Nanoparticles/nanotechnology . Simultaneous detection Introduction Inorganic contaminants, such as cadmium, arsenic, and sele- nium, pose a significant threat to human and ecological health due to their high toxicity and persistence in the environment. Cadmium is one of the most toxic heavy metals, arising from industrial wastes, phosphate fertilizers, smelting, and fuel combustion [1]. In the environment, Cd2+ is the dominant species and can irreversibly accumulate in the kidney, liver, lung, and pancreas of the human body, causing neurological, gastrointestinal, and skeletal illnesses [2]. The maximum con- taminant level (MCL), as set by the EPA for Cd2+ in drinking water, is 5.0 μg L−1 [3]. Arsenic is a poisonous chemical that is distributed widely in nature, ranked as twentieth in abun- dance among the elements in the earth’s crust [4]. Inorganic As3+, the most toxic form [4], is water-soluble and has been proven to cause many human health problems such as lung * Pradeep Kurup Pradeep_Kurup@uml.edu Dingnan Lu Dingnan_lu@student.uml.edu Connor Sullivan Connor_Sullivan1@student.uml.edu Eric M. Brack Eric.m.brack.civ@mail.mil Christopher P. Drew Christopher.p.drewphd.civ@mail.mil 1 Department of Civil and Environmental Engineering, University of Massachusetts Lowell, One University Ave., Lowell, MA 01854, USA 2 US Army Combat Capabilities Development Command Soldier Center (CCDC SC), General Greene Ave, Natick, MA 01760, USA Analytical and Bioanalytical Chemistry https://doi.org/10.1007/s00216-020-02642-4 http://crossmark.crossref.org/dialog/?doi=10.1007/s00216-020-02642-4&domain=pdf mailto:Pradeep_Kurup@uml.edu cancer and keratosis [5, 6]. The MCL of total arsenic allowed in drinking water is 10.0 μg L−1 [3]. Selenium is an essential element for animals, plants, and humans [7]. However, toxic effects have been observed in specific concentration ranges, and these effects can arise from an excess of this metalloid. Of the different oxidation states in which selenium can be found in nature (i.e., 4+, 6+, 0, and 2−), Se4+ is by far the most toxic form [8]. Furthermore, Se4+ is the only electroactive form of selenium [9]. The MCL of total selenium allowed in drinking water is 50.0 μg L−1 [3]. To address the environmental and health risks from these contaminants, it is important to devel- op a quick, sensitive, and accurate method for the detection of trace levels of Cd2+, As3+, and Se4+ in drinking water. Various analytical methods have been developed to de- tect different heavy metals in water samples, such as in- ductively coupled plasma-optical emission spectrometry (ICP-OES) [10–12], atomic absorption spectrometry (AAS) [13–15], inductively coupled plasma-mass spec- trometry (ICP-MS) [16, 17], and colorimetric and fluores- cence spectroscopy [18–20]. Although these methods have been proven to detect heavy metal accurately, some of the technologies mentioned above have significant drawbacks. For example, ICP-MS and ICP-OES require traditional centralized laboratories, expensive instruments, and highly trained technicians. Furthermore, AAS re- quires an additional gas supply to stimulate the optical radiation by gasified metal atoms. Fluorescence spectros- copy method needs a chemosensor or a biosensor equipped with a unique interaction mechanism for pro- voking or quenching the fluorescence effect when reacting with a specific heavy metal species, therefore preventing detection of multiple metal analytes, simulta- neously. Using anodic stripping voltammetry (ASV) for heavy metal detection in water is an attractive proposition due to the high sensitivity, low cost, and the potential application for onsite, simultaneous detection. Based on the comprehensive literature review, Cd2+, As3+, and Se4+ have been previously studied using ASV detection methods [9, 21, 22]. For example, Chow et al. [22] used a glutathione-modified gold electrode to perform electro- chemical detection of Cd2+ and reported a limit of detec- tion (LoD) of 5 nM. Toor et al. [21] successfully used an Au/Fe3O4 nanocomposite–modified glassy carbon elec- trode (GCE) to detect low levels of As3+ in water. Segura et al. [7] evaluated the performance of the gold nanoparticle (AuNP)–modified GCE on the detection of Se4+ and obtained a LoD of 0.12 ppb. It can be found that among all the electrode materials, gold-based electrodes showed superior performances on ASV detection of vari- ous heavy metal ions. In our previous study, nanoscale gold particles with a unique spiked geometry, referred to as gold nanostar (AuNS), have been proposed for im- proved ASV detection of Hg2+ and Pb2+ relative to traditional AuNPs with typically spherical geometry [23, 24]. In order to enlarge the applicability of the AuNS on ASV detection of heavy metals, it is necessary to develop new protocols for additional metal analytes, particularly cadmium, arsenic, and selenium. Simultaneous detection of multiple metal ions is one of the major growing trends of electrochemistry. For example, Ruecha et al. [25] used a graphene-polyaniline nanocomposite electrode to detect Zn2+, Cd2+, and Pb2+ in water simulta- neously. Mafa et al. [26] performed electrochemical co- detection of As3+, Hg2+, and Pb2+ on a bismuth-modified ex- foliated graphite electrode and achieved satisfactory detection sensitivity. Lu et al. [27] modified a GCE with CuZrO3/ graphene nanocomposite and used the modifiedGCE to detect Pb2+ and Cd2+ simultaneously. All of these studies showed the great potential and attractive prospect of electrochemical de- tection of multiple metal ions simultaneously. However, it should be noted that most of the published co-detection stud- ies only emphasized the fabrication of novel,sensitive elec- trodematerials while commonly overlooked the importance of having a suitable supporting electrolyte solution. In order to conduct ASV co-detection of multiple heavy metal ions, a universal supporting electrolyte must be developed in the first place, which should ideally possess a low background noise, a sizeable electrochemical window, and minimal environmental hazards. Based on the previously published studies, the peak locations of Cd2+, As3+, and Se4+ usually appear in a stripping voltammogram at three widely separated re- gions: Cd2+ at a highly negative potential [28–30], As3+ at a potential relatively close to 0 V [31–33], and Se4+ at a very positive potential [9, 34, 35]. Therefore, the most critical characteristic of a supporting electrolyte for ASV co-detection of Cd2+, As3+, and Se4+ is a broad electro- chemical window to ensure the precise observation of each ion’s stripping peak. To the best of our knowledge, such a universal supporting electrolyte has not been re- ported in the literature. A buffer solution, known as Britton-Robinson buffer (BRB), was previously devel- oped for colorimetric determination of [36]. This buffer consists of phosphoric acid, acetic acid, and boric acid, with an equal concentration of 0.04 M, providing a wide buffering range from pH 2 to 12. Compared with chloride, nitrate, and sulfate, present in commonly used supporting electrolytes, the anions (i.e., acetate, phosphate, and bo- rate) from BRB possess a low oxidizing ability, which can theoretically reduce the potential oxidation of gold nano- particle, thereby suppressing the formation of the unwant- ed gold oxidation peak when using a gold-based electrode to conduct ASV detection. Recently, the BRB has been used in electrochemical detection of different pharmaceu- tical compounds, such as atorvastatin [37], quinapril [38], sulfamethoxazole [39], and tinidazole [40]. However, Lu D. et al. there is scarce information on using the BRB as the supporting electrolyte for ASV detection of heavy metal ions. As a result, ASV detection of metal ions in the BRB or modified BRB (mBRB) is worthy of a detailed study. The first objective of the present study is to evaluate the feasibility of using the AuNS/SPCE (electrode) and mBRB (electrolyte) on electrochemical single detection of Cd2+, As3+, and Se4+. In the second part of this work, simultaneous detection of Cd2+, As3+, and Se4+ will be performed and fur- ther validated by comparing the detection performance with the conventional analytical method (i.e., atomic absorption spectrum). To the best of our knowledge, no attempt has been reported previously for the co-detection of cadmium, arsenic, and selenium using electrochemical detection method. Therefore, this study highlights the potential application of both AuNS/SPCE and mBRB for the simultaneous voltammetric detection of heavy metals in water. Experimental Reagents and apparatus All chemicals, purchased from Sigma-Aldrich, Inc., were of analytical reagent grade and used without further puri- fication. The mBRB solution was prepared by mixing equal amounts of stock solution of 0.1 M of phosphoric acid and acetic acid, resulting in a 0.1 M of pH 2.0 mBRB solution. Boric acid was excluded from the original BRB recipe since the original buffering capacity in the basic range is unnecessary in this study. Furthermore, boric acid has been shown in medical studies that its reproductive toxicity can cause male animals to suffer persistent testic- ular atrophy [41]. Therefore, removal of the boric acid reduced environmental and health risks associated with the test methodology. All voltammetric experiments were performed using a WaveNANO potentiostat (Pine Instruments, NC, USA) with the AfterMath software. All pH measurements were per- formed by a benchtop pH meter (AR15 Accumet™) with a gel-filled polymer body combination pH probe. A UV-Vis spectrophotometer (PerkinElmer LAMBDA 25) was used to perform UV-Vis measurements. Transmission electron mi- croscopy (TEM) images were obtained using the Philips EM400 T Microscope. HGA graphite furnace/atomic absorp- tion spectrum (AAS) (PerkinElmer PinAAcle 900T) was used to validate the results obtained by using the proposed voltammetric method. The X-ray diffraction (XRD) pattern was obtained using Rigaku RU-300E Diffractometer with Cu Kα radiation (λ = 0.1542 nm). The Fourier transform in- frared spectroscopy (FTIR) spectra were recorded using a NICOLET iS50 FT-IR with a scanning range of 500– 4000 cm−1. Preparation of gold nanostar suspension and electrode modification The gold nanostars were synthesized using the follow- ing procedure. A 0.1 M 4-(2-hydroxyethyl ) - l - piperazineethanesulfonic acid (HEPES) solution was first pre- pared, with the pH adjusted to 7.4 using 10M sodium hydrox- ide. The auric chloride solution was prepared by adding 30μL of 30% stock to 5 mL DI water, followed by heating in an oil bath at a constant temperature of 160 °C for 10 min. After heating, the chloroauric acid solution was capped and cooled to room temperature. Next, 2 mL of HEPES was mixed with 3 mL of DI water, and then, 50 μL of the freshly prepared auric chloride solution was added to it with mildly stirring. After mixing, the solution was left undisturbed while the outer spikes were forming. The solution turned light blue after 5 min and then darkened to a blue-green color in about 15 min. The final AuNS suspension was capped and stored in a dark temperature-controlled chamber at 10 °C. Screen-printed carbon electrodes (SPCEs) were used throughout the complete experiment, and all the SPCEs were obtained from Pine Instrumentation. The coating of the AuNS was performed first by wetting the surface of the working electrode with deionized water, following by pipetting the required volume (22 μL) of the AuNS solution onto the sur- face of the working electrode. The electrode was then placed in an oven at 40 °C overnight to dry the working electrode surface. After drying, the electrodes were removed from the oven and allowed to cool before testing. Titration study Titration was performed to quantify the buffering capacity of the mBRB. The experiments were performed by titrating 100 mL of the mBRB, made by mixing 50 mL of 0.1 M phosphoric acid and 50 mL 0.1 M acetic acid, with 0.2 N sodium hydroxide. pH measurements were made after the addition of each 2 mL of alkali. The pH values were recorded to plot the titration curve. Square wave anodic stripping voltammetry All voltammetric experiments were performed using square wave anodic stripping voltammetry (SWASV). The SWASV parameters were a deposition time of 180 s, a deposition po- tential of − 0.9 V, a stripping voltage range from − 0.9 to 0.9 V, an amplitude of 70 mV, a period of 20 ms, a step increment of 11 mV, and a sampling width of 5 ms. All measurements were carried out in triplicate. The limit of detection (LoD) was calculated using the following equation: LoD ¼ 3σ=m ð1Þ Simultaneous voltammetric detection of cadmium(II), arsenic(III), and selenium(IV) using gold... where σ is the standard deviation of replicate blank samples and m is the slope of the calibration curve. Results and discussion Characterization of AuNS and AuNS/SPCE TEM images were obtained to characterize the morphology and estimate the size of AuNS. As shown in the representative images (see Fig. 1), the average tip-to-tip diameter, average spike length, and average inner sphere diameter were approx- imately 49 ± 14 nm, 16 ± 1 nm, and 23 ± 6 nm, respectively. Furthermore, the number of spikes per nanostar ranged from 4 to 10. The XDR pattern of the obtained AuNS powder showed four diffraction peaks at 38.3°, 44.1°, 64.7°, and 77.3°, respec- tively. The observed four diffraction peaks (see Fig. 2a) were associated with the (111), (200), (220), and (311) Bragg re- flections, respectively, which are highly consistent with the XRD pattern of the standard crystalline gold XRD (JCPDS no. 04-0784), therefore confirming the crystallinenature of the prepared AuNS. The highest diffraction intensity recorded on the (111) plane suggests the predominant orientation among other planes. Thus, the average AuNS size was esti- mated based on the width of the (111) diffraction using the Debye-Scherrer equation [42]. The calculated mean size of the AuNS was found to be 40 nm, which is relatively in agree- ment with the TEM observation. FTIR analysis was carried out to demonstrate the presence of different organic functional groups on HEPES, which together can precisely exert the capping and stabilizing influence on the inner sphere of gold nanoparticles and eventually lead to the formation of nano- scale star-shaped crystalline gold. As shown in Fig. 2b, a weak band was found at approximately 1731 cm−1, which is asso- ciated with the presence of amide III on the HEPES molecule [43]. A relatively intense band is located at 1622 cm−1, which corresponds to the stretching vibration of the piperazine (1-(2- pyridyl)) ring [44]. Two intense bands observed at 1153 and 1022 cm−1 are assigned to the S=O stretching and pyridine breathing, respectively, and a sharp band at 661 cm−1 is mainly associated with the O=S=O in-plane deformation [44, 45]. It is worth mentioning that many early studies found the amide groups (I–III) can bind to gold nanoparticles and result in the stabilization of the bound gold nanoparticles [42, 43, 46–48]. Based on the obtained FTIR spectrum, it can be found that due to the presence of amide III, the selected cap- ping reagent of HEPES can impose a mild binding influence on the initially formed inner sphere of gold nanoparticles. The unique feature of the HEPES buffer allows the controlled growth of spherical gold nanoparticles, and eventually the formation of the AuNS. The UV-Vis spectra performed for the colorimetric charac- terization of the AuNS suspension are presented in Fig. 2c. The significant absorbance peak at 719 nm was associated with the outer spikes, and the relatively small absorbance peak at 521 nm was associated with the inner spherical cores. Eventually, the obtained AuNS showed a blue-green color (see Fig. 2c), which was mainly associated with the significant absorbance peak at 719 nm. As shown in Fig. 2d, electro- chemical impedance spectrum (EIS) tests were performed to investigate the behavior of AuNS/SPCE and SPCE in the presence of a redox probe (i.e., 10 mM Fe(CN)6 3−/4−). As the electrolyte resistance (RS) remained unchanged, the charge transfer resistance (RCT) decreased significantly from 2.4 kΩ (bare SPCE) to 0.8 kΩ (AuNS/SPCE). The differences ob- served in RCT can be ascribed to the increased surface area associated with the nanoscale AuNS coating on the working electrode surface. To directly estimate the effective surface area, cyclic voltammetry (CV) tests were performed in the presence of the same redox probe as used in the EIS tests (see Fig. 2e). Based on the Randle-Sevcik equation [49], the effective surface areas of AuNS/SPCE and SPCE can be cal- culated directly using the following equation: A ¼ IP= 2:69� 105 � n3=2D1=20 v1=2C � � ð2Þ where A is the effective electrode area (cm2), IP is the peak current (A), D0 is the standard diffusion coefficient of K3[Fe(CN)6] at 25 °C (cm 2/s), n is the number of electrons transferred in the redox event, v is the scan rate (V/s), and C is Fig. 1 Representative TEM images of AuNS Lu D. et al. the concentration of the redox species (mol (cm3)−1). The calculated effective surface areas of AuNS/SPCE and SPCE were 14.3 and 7.6 mm2, respectively, indicating the AuNS coating could approximately double the effective surface area of an unmodified SPCE electrode. Characterization of mBRB The titrant curve of mBRB (see Fig. 3) showed a pH buffering range from approximately 1.80 to 8.00. The linear regression line (R2 of 0.9921) indicated a strong correlation between the actual titration curve and the linear regression trendline. It is clear that the pKa values of phosphoric acid and acetic acid evenly distributed on the pH buffering range. Compared with that of the original BRB, the effective buffer range of mBRB is narrower, due to the exclusion of boric acid. Furthermore, as the concentrations of phosphoric acid and acetic acid are higher in themBRB (i.e., 50mM) than in the original BRB (i.e., 40mM), the slope of mBRB is more gradual than that of the original BRB, showing a better buffering capacity of mBRB. The AuNP/SPCE was used to evaluate the electrochemical window of the selected supporting electrolytes, including 50 mM mBRB, 50 mM HCl, 50 mM KCl, and 50 mM HAc/NaAc (pH 5.0) (see Fig. 4). The SWSAV technique was used with the corresponding parameters listed in the “Square wave anodic stripping voltammetry” section. Compared with the obtained baselines from all supporting electrolytes, the mBRB shows the broadest electrochemical window from approximated 0.8 to − 0.8 V, with the lowest background noise. Some unexpected noise peaks were ob- served in the voltammograms obtained in KCl and HCl at approximately 0.0 V, which are potentially associated with the Au0 anodically oxidizing to Au1+ in the presence of high chloride concentration (i.e., 0.05 M) [50, 51]. Furthermore, obvious hydrogen evolution occurred during the preconcentration step in HCl when having a deposition poten- tial of − 0.9 V. For practical applications, the deposition po- tential has to be reduced (i.e., less negative) to prevent the perturbing hydrogen evolution when applyingAVS in a strong acid like HCl, HNO3, and HClO4. However, the decrease of Fig. 2 a XRD pattern of AuNS power, b FTIR spectrum of AuNS/SPCE, c UV-Vis spectra of the AuNS suspension, d Nyquist plots, and e CV voltammograms obtained on AuNS/SPCE and bare SPCE in the presence of 10 mM Fe(CN)6 3−/4− and 0.1 M KCl Simultaneous voltammetric detection of cadmium(II), arsenic(III), and selenium(IV) using gold... the deposition potential will reduce the effectiveness of a preconcentration step, thereby reducing the sensitivity of the AVS detection of heavy metals. Acetate buffer (pH at approx- imately 5.0) is one of the most commonly used buffer systems for the simultaneous detection of multiple heavy ions [26, 30, 52]. As shown in Fig. 4d, the acetate buffer showed a flat and wide-open voltammogram from − 0.9 to 0.5 V. Within this potential segment, ions like Cd2+ and As3+ can clearly exhibit their oxidation peaks. However, the oxidation peak of Se4+ will be covered. Therefore, due to the large electrochemical window, small background noise, and the relatively low oper- ation risk, mBRB was selected as the supporting electrolyte for the following detection experiments. Individual detection of Cd2+, As3+, and Se4+ Cd2+, As3+, and Se4+ were first detected individually using AuNS/SPCE in 0.05 M of mBRB. Figure 5a shows the SWASV responses of Cd2+ over a concentration range of 0– 100 μg L−1. Well-defined stripping peak, linearly proportional to the spiked concentration of Cd2+, was observed at a poten- tial of − 0.48 V (versus Ag/AgCl). The linear regression equa- tion between peak current and analyte concentration is de- scribed as Eq. (3), with a correlation coefficient of 0.996. The limit of detection (LoD) was calculated to be 1.70 μg L−1 using Eq. 1. Next, the stripping peak of As3+ was located at − 0.1 V (versus Ag/AgCl), with relatively large Fig. 4 Electrochemical window of selected supporting electrolyte solutions: a 50 mM mBRB, b 5 mM KCl, c 50 mM HCl, and d 50 mM HAc/NaAc (pH 5.0) (electrode: AuNS/SPCE; SWASV parameter: deposition time of 180 s at − 0.9 V, stripping voltage range from − 0.9 to 0.9 V) Fig. 3 Titration curves of the original BRB (blue line) (adapted from Britton and Robinson [36]) and the modified BRB (red dashed line) Lu D. et al. peak height values when comparing with Cd2+. The responses of As3+ from 0 to 100 μg L−1 are shown in Fig. 5b. The equation of the linear regression is presented as Eq. (4), with its correlation coefficients of 0.998. The LoD was calculated tobe 0.49 μg L−1. The SWASV responses of Se4+ for the concentrations of 0, 25, 50, 75, and 150 μg L−1 are shown in Fig. 5c. The stripping peak of Se4+ was located at approx- imately 0.65 V (versus Ag/AgCl). The linear regression equa- tion is presented as Eq. (5), with the correlation coefficient of 0.996 and the LoD of 0.90 μg L−1. It should be noted that the observed anodic stripping peak of Se4+ is built partially on the left side of the gold anodic stripping peak at 0.85 V (versus Ag/AgCl), which resulted in the asymmetric profile of the Se4+ stripping peak [53]. i ¼ 0:0734 C þ 1:2828 ð3Þ i ¼ 0:225 C−0:4522 ð4Þ i ¼ 0:2213 C−4:8362 ð5Þ Simultaneous detection of Cd2+, As3+, and Se4+ The obtained ASV responses for the co-detection of Cd2+, As3+, and Se4+ with increasing concentrations under the opti- mal parameters are shown in Fig. 6a. The proposed electrodes (i.e., AuNS/SPCE) and supporting electrolyte (i.e., 0.05 mBRB) were applied successfully to the simultaneous deter- mination of the three target heavy metal ions. Cd2+, As3+, and Se4+ showed individual peaks at approximately − 0.48, − 0.09, and 0.65 V (versus Ag/AgCl), respectively. It is clear that the responses of three ions were well-separated in the stripping voltammogram. The stripping peaks of Cd2+ and Se4+ were located at the far ends of the electrochemical win- dow, with the As3+ stripping peak lying in between them. The separations among the three heavy metal ions are clear and large, which ensures the feasibility of simultaneous detection. It is worth noting that an additional open electrochemical win- dow is available from approximately 0 to 0.4 V, which may be suitable for adding mercury(II) [54] as another target heavy metal ion in the future. In Fig. 6b, the calibration curves of the Cd2+, As3+, and Se4+ co-detection were built from 0 to 100 μg L−1. For Cd2+, the linear regression equation is described as Eq. (6), with a correlation coefficient of 0.985 and a LoD of 1.62 μg L−1. Comparedwith the individual detection of Cd2+, simultaneous detection showed very similar results. Specifically, the slope of 0.0767 μA (μg L−1)−1 obtained from simultaneous detec- tion is slightly different from the individual detection result of 0.0734 μA (μg L−1)−1. In addition to the similar slopes ob- tained in the individual and simultaneous detection, the LoDs were also highly similar (i.e., 1.70 μg L−1 for individual de- tection and 1.62 μg L−1 for simultaneous detection). For As3+, the linear regression equation is described as Eq. (7) with a correlation coefficient of 0.996 and a LoD of 0.83 μg L−1. For Se4+, the linear regression equation is presented as Eq. (8), with a correlation coefficient of 0.989 and a LoD of 1.57 μg L−1. It is worth mentioning that, unlike Cd2+, both As3+ and Se4+ showed obvious decreases in their stripping peak height during the simul- taneous detection. Compared with the slopes obtained in the individual and simultaneous detections, As3+ and Se4+ showed apparent reductions of 40.8% and 42.7%, respec- tively. The decreased peak heights, observed in the As3+ and Se4+ co-detection, are likely due to the formation of insoluble arsenic triselenide (As2Se3). To the best of our knowledge, there is no previous research that performed ASV detection of As3+ and Se4+, simultaneously. Therefore, the potential mutual influence of As3+ and Fig. 5 SWASV response of the AuNS-modified SPCE for the individual detection of a Cd2+ over a concentration range of 0 to 100 μg L−1, bAs3+ over a concentration range of 0 to 100 μg L−1, and c Se4+ over a concen- tration range of 0 to 150 μg L−1 Simultaneous voltammetric detection of cadmium(II), arsenic(III), and selenium(IV) using gold... Se4+ was studied quantitatively to explain the observed decreased voltammetric responses in the following sec- tions. i ¼ 0:0767 C þ 1:0335 ð6Þ i ¼ 0:1331 C þ 0:5588 ð7Þ i ¼ 0:1267 C−1:4412 ð8Þ Evaluation of interaction between As3+ and Se4+ Figure 7a shows the significant differences in the observed stripping peak height when comparing individual and simul- taneous detection of 100 μg L−1 As3+ and Se4+. It was clear that both As3+ and Se4+ had a decreased peak height during co-detection. The average peak height of 100 μg L−1 of As3+ reduced from 21.73 ± 0.64 μA (individual) to 13.23 ± 0.25 μA (simultaneous), resulting in a peak height reduction of 39.1%. Similarly, the average peak height of Se4+ reduced from 17.34 ± 1.91 μA (individual) to 9.48 ± 0.37 μA (simul- taneous), showing a peak height reduction of 45.3%. The re- sults were highly consistent within the observations in the “Simultaneous detection of Cd2+, As3+, and Se4+” section, indicating the peak height reductions of As3+ and Se4+ have no direct relationship with the presence of Cd2+. Furthermore, Fig. 7b and c clearly show the stripping peaks of As3+ and Se4+ have no remarkable change when they are co-existing with Cd2+. As mentioned in the “Simultaneous detection of Cd2+, As3+, and Se4+” section, the possible cause of the peak height reductions of As3+ and Se4+ was associated with the formation of As2Se3. Since arsenic (0) tends to oxidize to arsenite triox- ide (As2O3) in the air at room temperature, and similar reac- tion to form arsenic triselenide can happen when zero-valent selenium is available [55], the relevant mechanisms can be described as follows: As3þ þ 3e−→As0 ð8Þ Se4þ þ 4e−→Se0 ð9Þ 2As0 þ 3Se0→As2Se3 ð10Þ The resultant of As2Se3 is highly stable and insoluble [56], which may cause the weakened stripping voltammetric re- sponse of As3+ and Se4+. For a better understanding of the observed peak height reductions, additional SWASVanalysis was performed over the concentration range of 0 to 100 μg L−1 when As3+ and Se4+ are co-existing (see Fig. 8). The standard addition analysis demonstrated the voltammetric responses of As3+ and Se4+ still increased linearly with the Fig. 6 a SWASV response of the AuNS-modified SPCE for the si- multaneous detection of cadmium(II), arsenic(III), and selenium(IV) over a concentra- tion range of 0 to 100 μg L−. b The calibration curves of cadmium(II), arsenic(III), and selenium(IV) simultaneous detection Lu D. et al. concentration increase, which was consistent with the results shown in the “Simultaneous detection of Cd2+, As3+, and Se4+” section. It should be noted that there is scarce informa- tion regarding the interaction between arsenic and selenium, and we are the first study reporting the decreased stripping peak heights during the co-detection of As3+ and Se−. However, it is reasonable to consider that the resultant As2Se3 is electrochemically inactive. Potential interferences and real water sample analysis Several common ionic species, typically present in ground and surface water [57, 58], were tested to evaluate the poten- tial interferences of the proposed detection method (see Table 1 for full results), specifically bicarbonate (HCO3 −), chlor ide (Cl−) , sulfate (SO4 2+) , i ron(III) (Fe3+) , magnesium(II) (Mg2+), and calcium(II) (Ca2+). Each species was testedwith 50μg L−1 of Cd2+, As3+, and Se4+ in triplicate. The average percent recovery (PR) and the relative standard deviation (RSD) were determined. It can be found that the PRs of each analyte during the different interference tests were generally above 90%, except for the results of the bicarbonate group (PR < 90%). In addition to the low PRs, the results of RSD obtained from the bicarbonate group were slightly larger than the results from other common ionic species. The obser- vations mentioned above together indicated that bicarbonate ion is a noticeable interference for this proposed detection method. As a common ion in groundwater, bicarbonate can react with acetic acid and phosphoric acid and consequently affect the system’s pH and ionic strength [59] as follows: NaHCO3 þ CH3COOH→CO2↑þ H2Oþ CH3COONa ð11Þ NaHCO3 þ H3PO4→CO2↑þ H2Oþ Na2HPO4 ð12Þ Two possible solutions to minimize the interference from bicarbonate ion are (1) diluting water samples (especiallya groundwater sample) to reduce the concentration of Fig. 7 a SWASV response of the individual and simultaneous detection of arsenic(III) and selenium(IV). b SWASV response of the individual and simultaneous detection of cadmium(III) and selenium(IV). c SWASV response of the individual and simultaneous detection of cadmium(III) and arsenic(IV) Fig. 8 SWASV response of the simultaneous detection of arsenic(III) and selenium(IV) over a concentration range of 0 to 100 μg L−1 Simultaneous voltammetric detection of cadmium(II), arsenic(III), and selenium(IV) using gold... bicarbonate ion and (2) increasing the concentrations of acetic acid and phosphoric acid to enhance the pH buffering capacity of the developed mBRB. Although the high concentration of bicarbonate ion can exert a moderate interference on the pro- posed method, the overall performance of the interference tests was acceptable (average PR ≥ 90%). Surface water was sampled and tested to evaluate the ana- lytical performance for real-world sample analysis. The water sample from the Merrimack River (Lowell, MA) was first filtered and preserved using 1 to 2 mL of concentrated nitric acid following the EPA standardmethod [60]. Before analysis, the pH of the preserved water sample was readjusted from 2.0 to 7.0 using 10 N sodium hydroxide. Without metal ion addi- tion, the water sample from theMerrimack River was found to contain non-detectable As3+ and Se4+, and this result was ver- ified by testing the same water sample using the AAS method (see Table 2). However, a trace Cd2+ concentration of 1.9 ± 0.2μg L−1 was observed in theMerrimack River sample using the proposed voltammetric method. This observation was highly consistent with the result of 2.2 μg L−1 obtained using the AAS detection method (graphite furnace mode). After spiking of 10 μg L−1 Cd2+, the proposed method resulted in a Cd2+ concentration of 12.0 ± 0.5 μg L−1, which again indi- cated an approximately 2.0 μg L−1 of Cd2+ found in the col- lected water sample. With simultaneous addition of all target ions at 10, 20, and 50 μg L−1, the proposed detection method resulted in average PRs of 109% for Cd2+, 93% for As3+, and 92% for Se4+, respectively. The results of surface water analysis demonstrated that the proposed method is accurate and reliable for the simultaneous detection of Cd2+, As3+, and Se4+ in real-world surface water samples. Reproducibility The reproducibility of the developed detection method was evaluated by measuring the voltammetric response of a solu- tion consisting of 50μg L−1 of Cd2+, As3+, and Se4+. Based on the results of five consecutive tests performed within 1 h, the RSD of each metal analytes was 5.7, 4.4, and 7.5% for Cd2+, As3+, and Se4+, respectively. Next, the peak heights of 50 μg L−1 of each ion obtained in five separate days resulted in the RSD of 6.5, 7.1, and 9.0% for Cd2+, As3+, and Se4+, respectively. Estimation of the storage tolerance for the devel- oped AuNS suspension is of interest. To evaluate that, 10 mL of AuNS suspension was kept in a clean glass vial at a temperature-controlled dark chamber at 10 °C for 3 months. After storage, the AuNS suspension was used directly to fabricate SPCEs, and the peak heights of all the metal analytes showed no significant reduction (difference less than 1%). The obtained RSD was 8.8, 7.9, and 10.4% for Cd2+, As3+, and Se4+, respectively. It is worth men- tioning that after an additional 1 month of storage, the AuNS suspension started to fade and exhibit some no- ticeable dark particles, which was associated with the long-term nanoscale collision and the following precip- itation of the AuNS particles. Table 2 Summary of surface water analysis Spiked (μg L−1) Proposed method (μg L−1) AAS method (μg L−1) PRa (%) Cd2+ As3+ Se4+ Cd2+ As3+ Se4+ Cd2+ As3+ Se4+ 0 1.9 ± 0.2 < LoD < LoD 2.2 ± 0.1 0.0 0.0 86b N/Ac N/Ac 10 12.0 ± 0.5 9.0 ± 0.8 8.9 ± 1.4 12.4 ± 0.3 9.6 ± 0.2 9.9 ± 0.3 120 90 89 20 21.7 ± 1.6 19.2 ± 2.1 18.7 ± 1.3 20.8 ± 0.1 19.5 ± 0.4 18.7 ± 0.3 108 96 94 50 49.7 ± 2.9 47.6 ± 2.4 45.9 ± 3.0 50.4 ± 0.5 48.9 ± 0.8 49.2 ± 0.5 99 95 92 a PR values calculated by comparing the results of the proposed method with spiked levels b PR of Cd2+ (w/o spike) calculated by comparing the results of the proposed method and AAS method cNot applicable Table 1 Summary of common interference testing with spiked 50 μg L−1 of each target ions Interference species Concentration (mg L−1) PRa of Cd2+ (%) PRa of As3+ (%) PRa of Se4+ (%) HCO3 − 200 87 ± 13 83 ± 17 84 ± 10 Cl− 500 103 ± 8 91 ± 8 92 ± 9 SO4 2+ 500 101 ± 5 98 ± 6 94 ± 7 Fe3+ 10 93 ± 7 88 ± 3 91 ± 5 Mg2+ 200 92 ± 3 96 ± 4 93 ± 5 Ca2+ 200 96 ± 6 93 ± 7 91 ± 7 aAverage percent recovery (PR) expressed as mean ± RSD of triplicate measurements Lu D. et al. Comparison with previous studies The detection performance of the proposed method was com- pared with other previously reported simultaneous detection studies, and results are presented in Table 3. Although the LoD obtained in this work is not the lowest, it is significantly lower than the EPA’s MCL of 5, 10, and 50 μg L−1 for cadmium(II), arsenic (total), and selenium (total) in drinking water, respectively [3]. It should be noted that the proposed method is the first work that includes Se4+ as a target analyte during simultaneous ASV detection. Furthermore, this pro- posed method has the potential of including more heavy metal ions, such as Hg2+, Pb2+, and Cu2+, as additional co-detection analytes. In comparison, the present work demonstrates a re- liable and versatile method for voltammetric detection of mul- tiple heavy metal ions simultaneously. Conclusion The gold nanostar (AuNS)–modified screen-printed carbon electrodes (SPCEs) and the modified Britton-Robinson buffer (mBRB) were used successfully to perform simultaneous voltammetric detection of cadmium(II), arsenic(III), and selenium(IV). The detection results suggested that (1) AuNS/SPCE can sensitively detect the three analytes, with LoD for Cd2+, As3+, and Se4+ of 1.6, 0.8, and 1.6 μg L−1, respectively; (2) 50 mM of pH 2.0 mBRB can provide a smooth and large electrochemical window that ensures all the ASV peaks to build up separately (peak location for Cd2+, As3+, and Se4+ are at − 0.48, − 0.09, and 0.65 V versus Ag/AgCl, respectively); (3) the peak heights of the three analytes increase linearly with increasing concentration. Furthermore, the results of simultaneous detection showed that the response of Cd2+ is independent of the presence of As3+ and Se4+. However, the co-existence of As3+ and Se4+ leads to the formation of electrochemically inactive arsenic triselenide (As2Se3) during the preconcentration period and consequently results in approximately 40% peak height reduc- tions for both As3+ and Se4+. Furthermore, the interferences and real water analyses showed that the proposed method could conduct reliable detection of Cd2+, As3+, and Se4+ si- multaneously in water. Funding information The authors received financial support from the U.S. Army Combat Capabilities Development Command – Soldier Center (Contract No. W911QY-17-2-0004) and the U.S. National Science Foundation Grant No. 1543042. Compliance with ethical standards No informed consent, human participants, and animals applicable. Conflict of interest The authors declare that they have no conflict of interest. Disclaimer Any opinions, findings, and conclusions or recom- mendations expressed in this manuscript are those of the authors and do not necessarily reflect the views of the National Science Foundation. Table 3 Summary of past efforts on the simultaneous ASV detection of heavy metal ions Electrode Electrolyte Target ions and LoD (μg L−1) Matrix analysis Ref MF/GCEa 10 mM NH4Ac/HCl; 5 mM NH4SCN Cd 2+ (0.06); Pb2+ (0.02) Seawater [29] AgREb 10 mM HNO3; 10 mM NaCl Cd 2+ (0.6); Pb2+ (0.08) Drinking water [28] Bi-EGEc 0.1 M acetate buffer (pH 5) Pb2+ (0.1); As3+ (0.02); Hg2+ (0.1) Wastewater [26] AuNPs/GCEd 0.1 M acetate buffer (pH 5) Cd2+(34); Pb2+ (62); Cu2+ (19); Hg2+ (60) – [52] BiBEe 0.1 M acetate buffer (pH 5) Zn2+ (0.4); Cd2+ (0.1); Pb2+ (0.1) River water [30] Gr/PANI/SPEf 1 M acetate buffer (pH 4.5) Zn2+ (1.0); Cd2+ (0.1); Pb2+ (0.1) Human serum [25] Au-Gr-Cys/Bi/GCEg 0.1 M acetate buffer (pH 4.5) Cd2+ (0.1); Pb2+ (0.05) Spring water [61] CuZrO3-Gr/GCEh 0.1 M acetate buffer (pH 4.6) Cd2+ (0.5); Pb2+ (0.1) Soil sample [27] AuNS/SPCE 50 mM mBRB (pH 2.0) Cd2+ (1.6); As3+ (0.8); Se4+ (1.6) River water This work aMF/GCE stands for mercury film–modified glassy carbon electrode bAgRE stands for silver rotating electrode c Bi-EGE stands for bismuth-modified exfoliated graphite electrode dAuNPs/GC stands for gold nanoparticle–modified glassy carbon electrode e BiBE stands for bismuth bulk electrode f Gr/PANI/SPE stands for graphene-polyaniline-modified screen-printed electrode gAu-Gr-Cys/Bi/GCE stands for gold nanoparticle-graphene-cysteine nanocomposite–modified bismuth film electrode h CuZrO3/Gr/GCE stands for copper zirconium oxide-graphene nanocomposite–modified glassy carbon electrode Simultaneous voltammetric detection of cadmium(II), arsenic(III), and selenium(IV) using gold... 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Abstract Introduction Experimental Reagents and apparatus Preparation of gold nanostar suspension and electrode modification Titration study Square wave anodic stripping voltammetry Results and discussion Characterization of AuNS and AuNS/�SPCE Characterization of mBRB Individual detection of Cd2+, As3+, and Se4+ Simultaneous detection of Cd2+, As3+, and Se4+ Evaluation of interaction between As3+ and Se4+ Potential interferences and real water sample analysis Reproducibility Comparison with previous studies Conclusion References
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