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Original article
2021
:14;
202103
doi:
10.1016/j.arabjc.2021.102990

Magnetic molecularly imprinting polymers and reduced graphene oxide modified electrochemical sensor for the selective and sensitive determination of luteolin in natural extract

Institute of Bast Fiber Crops, Chinese Academy of Agricultural Sciences, Changsha 410205, China

⁎Corresponding authors. liuliangliang@caas.cn (Liangliang Liu), huangsiqi@caas.cn (Siqi Huang)

Disclaimer:
This article was originally published by Elsevier and was migrated to Scientific Scholar after the change of Publisher.

Abstract

Abstract

The rapid and sensitive determination of luteolin was important since it was an effective antioxidant and bioactive supplement in food. For this purpose, magnetic molecularly imprinted polymer (Fe3O4@MIP) using luteolin as template was prepared, and then modified on the surface of glassy carbon electrode together with reduced graphene oxide (Fe3O4@MIP/rGO/GCE) for the sensitive electrochemical detection of luteolin. Through characterizations and adsorption experiments, Fe3O4@MIP demonstrated sphere structure with rough surface, well magnetic response in solution and better selectivity for luteolin than molecularly imprinted polymer (SiO2@MIP). After optimization of fabrication and electrochemical conditions, the Fe3O4@MIP/rGO/GCE exhibited satisfied anti-interference ability, linearity, detection limit, reproducibility and stability in detection. The linear detection range of luteolin using Fe3O4@MIP/rGO/GCE was from 2.5 pM to 0.1 μM, and the sensor could keep stable in six days. It was also successfully utilized in the determination of luteolin in lotus leaves extract with well recovery. Based on these results, the proposed electrochemical sensor Fe3O4@MIP/rGO/GCE had good prospects in evaluation of natural antioxidants.

Keywords

Electrochemical detection
Luteolin
Magnetic nanoparticles
Molecularly imprinted polymer
Reduced graphene oxide
1

1 Introduction

Luteolin was a crucial biological flavonoid widely distributed in various plants, seeds and fruits (Haminiuk et al., 2012). Many studies shown it has a wide range of pharmacological effects and could be used in the treatments of anti-inflammatory, anti-allergic, anti-tumor and anti-cancer (Gao et al., 2017; Pang et al., 2014). Due to extensively applications in pharmacology, it was a pressing problem to establish rapid, effective and reliable methods for the detection and pharmaceutical analysis of luteolin. On this basis, many methods were reported such as high performance liquid chromatography, gas chromatography, spectrophotometry, capillary electrophoresis and so on (Juszczak et al., 2019; Wei et al., 2019). However, there were some inherent disadvantages such as time consuming, high cost and complicated experimental operation in these methods. Electrochemical technology had strengths of simple operation, high sensitivity and fast response (Singh, 2016), and luteolin was an electroactive compound due to the catechol group on its B ring (Zuo, 2016). Hence, intensive studies in applicable electrochemical determination of luteolin were conducted and still noteworthy (Gao et al., 2020; Li et al., 2020).

As a kind of two-dimension nanomaterial, reduced graphene oxide (rGO) became an optimal material with large specific surface area, high chemical stability and electrochemical conductivity (Hu et al., 2016; Sugimoto et al., 2020). It was often used to fabricate electrochemical sensors with enhanced performance in detection and catalysis with single component alone and combination of other materials (Ratinac et al., 2011; Rowley-Neale et al., 2018).

Molecular imprinting polymer (MIP) had the recognition property of template because of the multiple binding sites formed between template molecules and monomers (Wackerlig and Lieberzeit, 2015). Accordingly, it exhibited unique high selectivity and structural predictability during separation, purification and determination of template molecules in food and environmental fields (Bi et al., 2013). Especially in electrochemical analysis, MIP modified electrochemical sensor exhibited higher sensitivity and selectivity than traditional sensors (El Nashar et al., 2017; Fu et al., 2019). With the development of nanotechnology, combinations of MIP with other nanomaterials were designed and achieved good results (Gui et al., 2019; Jin et al., 2018). This kind of compositions exhibited a synergic effect that signal improvements and mechanical characteristics (Amatatongchai et al., 2020; Gui et al., 2018).

Many kinds of nanomaterials were used in the modification of glassy carbon electrode (GCE) and gold electrode for the detection of luteolin (Cheng et al., 2020; Liu et al., 2019a,b,c). Several MIP modified electrode using luteolin as template through electropolymerization were proposed by Zeng and Du as well (Wei et al., 2019; Xu et al., 2017). However, the modifications of magnetic MIP (MIP using Fe3O4 magnetic nanoparticles as core, Fe3O4@MIP) and rGO on GCE for detection of luteolin was not reported. In this study, Fe3O4@MIP nanomaterials were prepared using luteolin as templates to improve the selectivity and electrical conductivity for application in electrochemical sensing of luteolin. The selectivity and signal enhancement were evaluated and compared with MIP prepared using silica nanoparticles as core materials (SiO2@MIP). Fe3O4@MIP showed better signal improvement, adsorption capacity and selectivity for luteolin than those of SiO2@MIP. Then, rGO and Fe3O4@MIP were successively modified on GCE (Fe3O4@MIP/rGO/GCE) to develop a simple, sensitive and specific sensor for detection of luteolin (Fig. 1). The prepared Fe3O4@MIP and rGO were characterized by transmission electron microscopy (TEM), scanning electron microscopy (SEM), Fourier transform infrared (FT-IR) spectra and vibration sample magnetometer (VSM). Under the optimized preparation and analytical conditions, Fe3O4@MIP/rGO/GCE demonstrated good enhancements in the selectivity and electrochemical signal, satisfied anti-interference, linearity and low detection limit for luteolin. The good performance of Fe3O4@MIP/rGO/GCE made this kind of electrochemical sensor having good application prospects in natural antioxidants evaluations in food and analytical fields.

The fabrication of Fe3O4@MIP/rGO/GCE for the electrochemical detection of luteolin.
Fig. 1
The fabrication of Fe3O4@MIP/rGO/GCE for the electrochemical detection of luteolin.

2

2 Materials and methods

2.1

2.1 Reagents

Luteolin (>98.0%), tetraethyl orthosilicate (TEOS, >97.0%), methacrylic acid (MAA), 4-vinylpyridine (4-VP), acrylamide (AM), acrylic acid (AA), ethyleneglycol dimethacrylate (EGDMA), 3-methacryloxypropyltrimethoxysilane (MPS, KH570) and azodiisobutyronitrile (AIBN) were bought from TCI (Shanghai) Development Co., Ltd. (Shanghai, China). Graphite flakes was purchased from Nanjing XFNANO Materials Tech Co., Ltd (Nanjing, China). Potassium permanganate, ferric chloride, sodium acetate, polyethylene glycol (PEG) 6000, and potassium ferricyanide were obtained from Sinopharm Chemical Reagent Co., Ltd. (Shanghai, China). Dry lotus leaves were bought from Qinyuan Chinese medicines company (Bozhou, China). All aqueous solutions were prepared with deionized water supplied by an ELGA water purification system (ELGA Berkefeld, Veolia, Germany). All other chemicals were bought from Sinopharm Chemical Reagent Co., Ltd. (Shanghai, China) with analytical grade.

2.2

2.2 Preparation of Fe3O4@MIP and SiO2@MIP

Fe3O4 magnetic nanoparticles, SiO2 nanoparticles and rGO were prepared according to previous reports and shown in Supplementary Information (SI) (Cen et al., 2017; Liu et al., 2019a,b,c; Orooji et al., 2020). The core nanoparticles (Fe3O4 and SiO2) were firstly modified with MPS. 0.60 g of core nanoparticles were dispersed in 100 mL of ethanol and treated by ultrasonication for 30 min. Then, 5 mL of MPS were slowly added under mechanical stirring and the mixture was reacted at room temperature for 24 h. The products (Fe3O4@MPS and SiO2@MPS) were collected by a magnet or centrifugation, washed with ethanol and stored for further use.

For polymerization, 0.3 mmol of luteolin and 1.8 mmol of MAA were preincubated in 30 mL of acetonitrile for 12 h under magnetic stirring in ice bath. 0.50 g of Fe3O4@MPS or SiO2@MPS, 5.4 mmol of EGDMA and 50 mg of AIBN were dispersed in 100 mL of acetonitrile. The dispersion was submitted to ultrasonication for 30 min, mixed with template solution, bubbled by nitrogen gas for 5 min and reacted at 50 °C for 6 h and 60 °C for 24 h. After polymerization reaction, the products (Fe3O4@MIP and SiO2@MIP) were collected and washed with acetonitrile. Finally, Fe3O4@MIP and SiO2@MIP were refluxed in methanol using Soxhlet extraction for 24 h and collected for further use. For comparison, non-imprinted polymer using Fe3O4 magnetic nanoparticles as core materials (Fe3O4@NIP) was prepared according to the same procedures except the absence of template. The Fe3O4@MIP and SiO2@MIP were characterized by TEM, SEM, FT-IR and VSM with detail equipment information shown in SI.

2.3

2.3 Adsorption of luteolin using Fe3O4@MIP and SiO2@MIP

The adsorptions of luteolin were performed using Fe3O4@MIP and SiO2@MIP for comparing the selectivity and adsorption capacity (Liu et al., 2019a,b,c). 30 mg of Fe3O4@MIP or SiO2@MIP was suspended into 5 mL of luteolin methanol solution (0.1 M) and shaken for 30 min at room temperature. After adsorption, Fe3O4@MIP was separated by a magnet and SiO2@MIP was separated by centrifuge. Then, the change in adsorptions of luteolin solution was detected by a spectrophotometer at 350 nm (UV-2700 Shimadzu, Kyoto, Japan). The concentrations of luteolin were determined by a standard curve and the adsorption capacity of luteolin was calculated according to following formula:

(1)
Adsorption capacity = C 0 - C / C 0 × 100 % where C0 and C are the concentration of luteolin before and after adsorption.

2.4

2.4 Fabrication of Fe3O4@MIP/rGO/GCE

Before the modification of GCE, the electrode was polished with alumina powders, washed with water and ultrasonic treated for 5 min. The water on surface of GCE was drying with nitrogen gas and stored for modifications. rGO and Fe3O4@MIP (5 mg mL−1) suspensions were respectively treated by ultrasonication for 30 min. Firstly, 9 μL of rGO suspension was dripped on the fresh polished electrode surface, dried in the air and marked as rGO/GCE. Then, 7 μL of Fe3O4@MIP suspension was dripped on the surface of rGO/GCE and dried in the air, which was termed as Fe3O4@MIP/rGO/GCE. For comparison test, the same amount of Fe3O4@MIP was directly modified on fresh polished GCE under the same procedures and marked as Fe3O4@MIP/GCE.

2.5

2.5 Electrochemical measurements

The electrochemical measurements in this experiment were conducted by a CHI660E electrochemical workstation (Shanghai Chenhua Instrument Co., Ltd., Shanghai, China) with a standard three-electrode system: an Ag/AgCl electrode as the reference, a platinum wire as the auxiliary, and a bare or modified GCE as the working electrode. The three-electrode system was immersed in phosphate buffer saline (PBS) as supporting electrolyte containing luteolin or other solutes. The measurements were performed using cyclic voltammetry (CV) with the potential range from −0.2 V to 1.0 V and scan rate of 10 mV s−1, and differential pulse voltammetry (DPV) with the potential range from −0.2 V to 0.6 V, scan rate of 10 mV s−1, pulse amplitude of 50 mV and pulse width of 50 ms. All measurements were completed at room temperature (25 ± 2 °C) with three replications.

2.6

2.6 Preparation of real sample

50.0 g of lotus leaves were ground, soaked in 200 mL of methanol solution (70%, v: v) and reflux extracted at 85 °C for 2 h. Then, the solution was cooled to room temperature, filtrated and stored at 4 °C. Before detection, 10 μL of sample solution was diluted to 100 mL with PBS for determination.

3

3 Results and discussion

3.1

3.1 Characterizations of Fe3O4@MIP and rGO

3.1.1

3.1.1 TEM and SEM

The structures and morphologies of rGO, Fe3O4 magnetic nanoparticles and Fe3O4@MIP were characterized by TEM and SEM. In Fig. 2a, rGO showed typical characters of two-dimension nanomaterials like translucent and wrinkled edges. The prepared Fe3O4 magnetic nanoparticles were black spheres with diameters at about 400 nm (Fig. 2b) (Chen et al., 2017). After polymerization, Fe3O4@MIP showed similar sphere structure and the surface became rougher and more porous (Fig. 2c), which might be caused by molecular imprinting and elution of templates. SEM image of Fe3O4@MIP was presented in Fig. 2d as well. It could be seen that the spherical polymers were distributed with uniform size. The morphology observed in SEM image was in an agreement with those in TEM image, and the size distribution of Fe3O4@MIP in a wider range was clearly displayed. Hence, spherical Fe3O4@MIP was successfully prepared with uniform size and well dispersion.

TEM images of (a) rGO, (b) Fe3O4 magnetic nanoparticles and (c) Fe3O4@MIP; (d) SEM image of Fe3O4@MIP.
Fig. 2
TEM images of (a) rGO, (b) Fe3O4 magnetic nanoparticles and (c) Fe3O4@MIP; (d) SEM image of Fe3O4@MIP.

3.1.2

3.1.2 FT-Ir

FT-IR spectra of Fe3O4 magnetic nanoparticles, SiO2 nanoparticles, Fe3O4@MIP and SiO2@MIP were conducted. As shown in Fig. 3a, both Fe3O4 magnetic nanoparticles and Fe3O4@MIP exhibited a typical absorption at 584 cm−1 in their spectra, which was assigned to Fe-O stretching vibration and indicated the existence of Fe3O4 magnetic nanoparticles (Liu et al., 2013). While, SiO2 nanoparticles and SiO2@MIP showed some bands at 474 cm−1, 1103 cm−1 and 3432 cm−1, which were attributed to vibration network of O-Si-O, irregular stretching vibration of Si-O and O-H stretching vibration from silanol groups (Imoisili et al., 2020). It could be found the band at 3432 cm−1 increased after polymerization from Fe3O4 magnetic nanoparticles to Fe3O4@MIP (from SiO2 nanoparticles to SiO2@MIP), which might because more oxygen molecules were modified on the nanoparticles and related O-H vibrations enhanced (Hatamluyi et al., 2020).

(a) FT-IR spectra of Fe3O4 magnetic nanoparticles, SiO2 nanoparticles, Fe3O4@MIP and SiO2@MIP; (b) Magnetization curves of Fe3O4 magnetic nanoparticles and Fe3O4@MIP.
Fig. 3
(a) FT-IR spectra of Fe3O4 magnetic nanoparticles, SiO2 nanoparticles, Fe3O4@MIP and SiO2@MIP; (b) Magnetization curves of Fe3O4 magnetic nanoparticles and Fe3O4@MIP.

3.1.3

3.1.3 Vsm

In order to evaluate the magnetic response property, the magnetization curves of Fe3O4 magnetic nanoparticles and Fe3O4@MIP were characterized and plotted in Fig. 3b. It could be found the maximum saturation magnetization of Fe3O4 magnetic nanoparticles was 63.3 emu g−1, and then this value of Fe3O4@MIP reduced to 49.1 emu g−1. This kind of reduction was familiar in modification of magnetic materials and attributed to the existence of nonmagnetic coating after polymerization (Liu et al., 2019a,b,c). However, Fe3O4@MIP was still sufficient for magnetic separation with ordinary magnets. It could be easily separated in solution within 2 min, which indicated that Fe3O4@MIP simplified the procedures and could be used in further experiments.

3.2

3.2 Optimization of preparation conditions of Fe3O4@MIP

3.2.1

3.2.1 Effect of monomer

Proper monomer could make a stable complex through binding to template molecules, which was conducive to the following polymerization. Accordingly, four typical monomers (MAA, 4-VP, AM and AA) were selected in the preparation of Fe3O4@MIP. The adsorption capacities of resulting polymers were compared and shown in Fig. 4a, four kinds of Fe3O4@MIP exhibited various adsorption capacities for luteolin. Among them, Fe3O4@MIP prepared using MAA had the maximum adsorption capacity, which might due to MAA could contribute to stronger molecular interactions with the template molecules than other monomers (Yang et al., 2020). Therefore, MAA was selected as the monomer for preparation of Fe3O4@MIP.

(a) Effect of monomer ratio on adsorption capacity, (b) Effect of mole ratio of template, monomer and crosslinker on adsorption capacity and (c) adsorption performances of Fe3O4@MIP, SiO2@MIP and Fe3O4@NIP.
Fig. 4
(a) Effect of monomer ratio on adsorption capacity, (b) Effect of mole ratio of template, monomer and crosslinker on adsorption capacity and (c) adsorption performances of Fe3O4@MIP, SiO2@MIP and Fe3O4@NIP.

3.2.2

3.2.2 Effect of mole ratios of template, monomer and crosslinker

In preparation of MIP, the amounts of template, monomer and crosslinker would affect the structures and adsorption abilities of resultant polymers. The effects of mole ratio of luteolin to MAA (1:2, 1:4, 1:6), and mole ratio of MAA to EGDMA (1:1, 1:3, 1:5) were conducted. The adsorption capacities of nine Fe3O4@MIP under the various ratios of template, monomer and crosslinker (1:2:2, 1:4:4, 1:6:6, 1:2:6, 1:4:12, 1:6:18, 1:2:10, 1:4:20 and 1:6:30) were shown in Fig. 4b. As a result, Fe3O4@MIP with ratio of 1:6:18 exhibited the maximum adsorption capacity for luteolin. The optimal mole ratio of luteolin to MAA (1:6) was in accordance with report, which indicated the mole ratio would change the number of active binding sites and film thickness, leading to the influence on electronic conductive property (Yang et al., 2017). Therefore, the mole ratios of luteolin, MAA and EGDMA were determined as 1:6:18.

3.2.3

3.2.3 Adsorption performances of Fe3O4@MIP and SiO2@MIP

In order to compare the selectivity and adsorption capacities of Fe3O4@MIP, SiO2@MIP and Fe3O4@NIP, three structural analogues along with luteolin were used as adsorption targets. During adsorption experiments, the concentrations of luteolin and structural analogues were the same, and the calculations were proceed using their own standard curves. As illustrated in Fig. 4c, both Fe3O4@MIP and SiO2@MIP had the maximum adsorption capacity for luteolin. While, there was no specific adsorptions of Fe3O4@NIP among these four targets, which indicated the MIP was effective in specific adsorption of luteolin. For Fe3O4@MIP, the adsorption capacity of luteolin was 25.6 times that of catechin, 3.2 times that of p-hydroxybenzoic acid and 6.1 times that of puerarin. For SiO2@MIP, the adsorption capacity of luteolin was 3.7 times that of catechin, 2.2 times that of p-hydroxybenzoic acid and 2.7 times that of puerarin. It demonstrated Fe3O4@MIP had a high selectivity for luteolin than that of SiO2@MIP. Therefore, the adsorption performances of Fe3O4@MIP indicated that it had a good recognition and adsorption capacity for luteolin.

3.3

3.3 Electrochemical properties of modified electrodes

The electrochemical responses of luteolin on several modified electrodes were compared and shown in Fig. 5. The peak current was only 0.50 μA on bare GCE for 1.0 μM of luteolin. For the same concentration of luteolin, the modifications of rGO and Fe3O4@MIP respectively increased the peak current to 3.11 μA and 3.37 μA. These enhancements could be attribute to the large surface area, adsorption ability and electronic conductivity of rGO and the selectivity and enrichment of Fe3O4@MIP (Ross and Civilized Nqakala, 2020; Tang et al., 2020). While, the peak current of luteolin on Fe3O4@MIP/rGO/GCE reached 10.52 μA, which was 21 times higher than that on bare GCE. Compared with Fe3O4@MIP/rGO/GCE, the signal on SiO2@MIP/rGO/GCE was moderate (3.05 μA). This comparison indicated the conductivity of core material was important to electrochemical signal of modified electrode, and Fe3O4@MIP made an improvement on signal for luteolin. The combination of rGO and Fe3O4@MIP in the modifications exhibited a synergic effect on signal improvement, which was mentioned in previous report (Amatatongchai et al., 2020). Accordingly, Fe3O4@MIP/rGO/GCE was selected as an electrochemical sensor for luteolin among these modified electrodes with the highest electrochemical signal.

DPV in luteolin solution with bare GCE, Fe3O4@MIP/GCE, rGO/GCE, SiO2@MIP/rGO/GCE and Fe3O4@MIP/rGO/GCE.
Fig. 5
DPV in luteolin solution with bare GCE, Fe3O4@MIP/GCE, rGO/GCE, SiO2@MIP/rGO/GCE and Fe3O4@MIP/rGO/GCE.

3.4

3.4 Optimization of electrochemical conditions

3.4.1

3.4.1 Effect of pH

In order to confirm the optimum pH value of electrolyte, different pH values of electrolyte from 4.0 to 9.0 were investigated by detection of luteolin with DPV using Fe3O4@MIP/rGO/GCE. As shown in Fig. 6a, the peak current reached the maximum value when pH was 7.0. In both acidic and alkaline electrolytes, the peak current showed decreases. Insufficient protons in solution at high pH could made the electrochemical reaction difficult. Moreover, luteolin would converted into anion status resulting electrostatic repulsion between luteolin anions and negative ions on electrode (Liu et al., 2019a,b,c; Xie et al., 2020). Hence, the pH value of electrolyte during test was set at 7.0.

(a) Effect of pH values on peak current of luteolin in DPV; (b) Effect of modification volumes of rGO on peak current of luteolin in DPV; (c) Effect of modification volumes of Fe3O4@MIP on peak current of luteolin in DPV; (d) CV of Fe3O4@MIP/rGO/GCE in luteolin solution at different scan rates; (e) DPV of Fe3O4@MIP/rGO/GCE in different concentrations of luteolin solution; (f) Plot of peak current versus concentration of luteolin in logarithmic form.
Fig. 6
(a) Effect of pH values on peak current of luteolin in DPV; (b) Effect of modification volumes of rGO on peak current of luteolin in DPV; (c) Effect of modification volumes of Fe3O4@MIP on peak current of luteolin in DPV; (d) CV of Fe3O4@MIP/rGO/GCE in luteolin solution at different scan rates; (e) DPV of Fe3O4@MIP/rGO/GCE in different concentrations of luteolin solution; (f) Plot of peak current versus concentration of luteolin in logarithmic form.

3.4.2

3.4.2 Effect of modification volumes of rGO and Fe3O4@MIP

Effects of modification volumes of rGO (from 5 μL to 10 μL) and Fe3O4@MIP (from 4 μL to 9 μL) were conducted to optimize the modification amounts of two materials. The concentrations of rGO and Fe3O4@MIP were 5.0 mg mL−1. Firstly, the modification volume of rGO was investigated and shown in Fig. 6b. The peak current increased with increasing modification volume of rGO until the volume reached 9 μL. More volume of rGO like 10 μL reduced the current sharply. Then, after modification with 9 μL of rGO, the modification volume of Fe3O4@MIP was examined. With similar trends, the peak current reached the highest value when the modification volume of Fe3O4@MIP was 7 μL, and then decreased when the volume was more than 7 μL (Fig. 6c). Therefore, the modification volumes of rGO and Fe3O4@MIP were optimized at 9 μL and 7 μL, respectively.

3.4.3

3.4.3 Effect of scan rate

The effect of scan rate (from 0.01 V s−1 to 0.3 V s−1) on the electrochemical signals was investigated by detection of luteolin with CV using Fe3O4@MIP/rGO/GCE. As shown in Fig. 6d, the peak currents in CV were getting higher with increasing scan rate. A linear change could be found between peak current and scan rate, which could be fitted as: Ipa = 16.61 v + 0.3512 (r2 = 0.994) (Fig. S1 in SI). The linear increasing of peak current indicated that the redox reaction occurred on the surface of Fe3O4@MIP/rGO/GCE was controlled by adsorption process (Yuan et al., 2020). Despite the higher signals during increasing scan rate, the fluctuation and signal-to-noise ratio were more apparent as well. Therefore, the scan rate was controlled at 0.05 V s−1 during test considering these influences together.

3.5

3.5 Quantitative analysis of luteolin

After the optimization of electrochemical conditions, the quantitative analysis of luteolin with DPV using Fe3O4@MIP/rGO/GCE was performed at concentrations ranged from 2.5 pM to 0.1 μM (Fig. 6e). As a result, the peak currents increased linearly with the logarithmic increase of luteolin. The linear equation concerned the peak currents and concentrations could be fitted as: y = 0.301 logC + 2.287 (r2 = 0.995) (Fig. 6f). The limit of detection of luteolin reached 1 pM. Through the comparison of reported modified electrodes in detection of luteolin, the Fe3O4@MIP/rGO/GCE proposed in this study exhibited good linearity and low detection limit (Table S1 in SI).

3.6

3.6 Anti-interference, reproducibility and stability

For anti-interference ability of Fe3O4@MIP/rGO/GCE, some substances (NaCl, KCl, CaCl2 and tectorigenin) were added into luteolin solution and detected with DPV. The concentrations of these interferents were 5000 times higher than that of luteolin. In order to evaluate the anti-interference ability of Fe3O4@MIP/rGO/GCE, the current ratio (%) was calculated as the ratio of peak current variation and original current value during the addition of interferent (Singh et al., 2020). As illustrated in Fig. 7a, the current ratio was from 1.4% to 2.7%, indicating the influence of interferents on the detection of luteolin was limited. When the same amount of luteolin was added, the current ratio was about 103.8%, which demonstrated the detection of luteolin was reliable.

(a) Peak current ratio of Fe3O4@MIP/rGO/GCE in luteolin containing interfering substances; (b) Reproducibility and (c) stability of Fe3O4@MIP/rGO/GCE in luteolin solution.
Fig. 7
(a) Peak current ratio of Fe3O4@MIP/rGO/GCE in luteolin containing interfering substances; (b) Reproducibility and (c) stability of Fe3O4@MIP/rGO/GCE in luteolin solution.

For reproducibility of Fe3O4@MIP/rGO/GCE, the peak currents of luteolin in DPV using the same electrode six times a day were monitored. It could be found in Fig. 7b that the results were stable with relative standard deviation at 4.23% (n = 6). The stability of Fe3O4@MIP/rGO/GCE was also investigated by consecutively detecting the peak currents of luteolin in DPV using the same electrode in six days (Fig. 7c). The relative standard deviation for stability test (n = 6) was just 4.67%. Therefore, the electrochemical detection of luteolin using Fe3O4@MIP/rGO/GCE showed anti-interference ability to some interferents, reproducibility and stability of results.

3.7

3.7 Determination of luteolin in real samples

In order to estimate the practicality of Fe3O4@MIP/rGO/GCE, the detection of luteolin in real samples were conducted, and the recovery test during detection was also carried out by standard addition method. As expressed in Table 1, there was 42.4 ± 0.5 nM of luteolin in lotus leaves extract and the recoveries in detection were ranged from 98.5% to 100.7%. Moreover, the relative standard deviation values were less than 1.24%. Therefore, the Fe3O4@MIP/rGO/GCE showed well detection of luteolin in real samples with satisfied recovery and accuracy.

Table 1 Determination of luteolin in lotus leaves sample (n = 3).
Samples Added (nM) Found (nM) Recovery (%) RSD (%)
Lotus leaves extract 42.4 ± 0.5 1.06
5 47.3 ± 0.4 99.3 0.85
10 52.4 ± 0.6 100.7 1.24
20 62.1 ± 0.3 98.5 0.41

4

4 Conclusions

In this study, Fe3O4@MIP was prepared using luteolin as template under the optimal mole ratio of reactants. Compared with SiO2@MIP, Fe3O4@MIP showed better adsorption performance and signal enhancement. With good selectivity and signal enhancement, Fe3O4@MIP and rGO were successively modified on GCE (Fe3O4@MIP/rGO/GCE) to develop a simple, high sensitivity and selectivity sensor for detection of luteolin. The modifications of Fe3O4@MIP and rGO exhibited the most enhancement than single modification and bare GCE. After optimization of fabrication and detection conditions, the Fe3O4@MIP/rGO/GCE demonstrated satisfied anti-interference, linearity, detection limit, reproducibility and stability for luteolin. The linear range reached from 2.5 pM to 0.1 μM with detection limit at 1 pM and the relative standard deviations in reproducibility and stability were lower than 4.7%. With well recovery in determination of luteolin in natural extract, Fe3O4@MIP/rGO/GCE could be further developed as a practical sensitive sensor for the applications in natural antioxidants evaluations in food and analytical fields.

Acknowledgments

This work was supported by the Central Public-interest Scientific Institution Basal Research Fund (No. 1610242020005), Open project of key laboratory of biology and processing for bast fiber crops, MARA, and National Agricultural Science and Technology Innovation Project and Genetic breeding and quality safety assessment of Southern characteristic fruit trees, CAAS-ASTIP-21-IBFC10 (Characteristic fruit and vegetable innovation team, ASTIP-IBFC05).

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

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Appendix A

Supplementary material

Supplementary data to this article can be found online at https://doi.org/10.1016/j.arabjc.2021.102990.

Appendix A

Supplementary material

The following are the Supplementary data to this article:

Supplementary data 1

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