Natalia Manousia,
Eleni A. Deliyannib,
Erwin Rosenberg*c and
George A. Zachariadisa
aLaboratory of Analytical Chemistry, Department of Chemistry, Aristotle University of Thessaloniki, Thessaloniki 54124, Greece
bLaboratory of Chemical and Environmental Technology, Department of Chemistry, Aristotle University of Thessaloniki, Thessaloniki 54124, Greece
cInstitute of Chemical Technologies and Analytics, Vienna University of Technology, Getreidemarkt 9/164, 1060 Vienna, Austria. E-mail: erwin.rosenberg@tuwien.ac.at
First published on 28th May 2021
A novel micro–meso porous activated carbon/Fe3O4 (Bm) composite was synthesized from the active charcoal precursor BAX-1500 and used in the magnetic solid-phase extraction (MSPE) of caffeine prior to its determination by gas chromatography-mass spectrometry (GC-MS). The main factors affecting the extraction and desorption steps of the MSPE procedure were investigated and optimized. These factors include extraction time, sorbent mass and salt addition for the adsorption step and type of eluent, desorption time and volume of desorption solution for the desorption step. Under optimum conditions, the absolute extraction recovery was found to be 91.1% and good linearity was observed in the investigated concentration range of 0.6–12.5 ng mL−1 (R2 = 0.9997). The limit of detection was 0.18 ng mL−1 and the limit of quantification was 0.60 ng mL−1. The method was successfully applied to the analysis of surface water samples. The proposed MSPE method is simple, rapid, sensitive and environmentally friendly.
Caffeine is an alkaloid that is constituent of a variety of foods (chocolate, pastries etc.) and beverages (coffee, tea, soft drinks). Caffeine is a useful potential chemical marker for the estimation of domestic human wastewater contamination. Therefore, the determination of caffeine in surface water samples is critical to evaluate the impact of anthropogenic activity for waste water contamination of surface water. Since the concentration of caffeine in surface water may be low, preconcentration is considered a necessary step in sample preparation.5,6
Caffeine is usually determined by high performance liquid chromatography (HPLC) combined with a variety of detection systems including ultraviolet (UV),7 diode array detection (DAD)8 and mass spectrometry (MS).9 However, HPLC analysis may involve the use of hazardous solvents as mobile phases, plus the inconvenience of buffer preparation for pH adjustment. Gas chromatography (GC) can be applied to avoid these time- and cost-consuming steps and is also environmentally more benign.10 Therefore gas chromatography combined with a flame ionization detector (FID)10 or mass spectrometer11 has been successfully employed for the determination of caffeine in a variety of matrices. Until now, solid-phase extraction (SPE)12 and liquid–liquid extraction (LLE)13 are the two major conventional sample preparation techniques that are used for the extraction of caffeine from a plethora of samples. However, these techniques exhibit some fundamental limitations since they comprise of time-consuming steps and they require the consumption of high quantities of sample and organic solvents.14 Compared to the conventional methods for the determination of caffeine, MSPE is rapid and a convenient choice.
Various magnetic sorbents have been employed for the magnetic solid-phase extraction including activated carbon,15 metal–organic frameworks,16 molecularly imprinted polymers17 and graphene oxide.4 Activated carbon exhibits high surface area, a wide range of surface functional groups and internal microporosity, therefore it has proved to be an effective sorbent that can be used for the separation and purification of gaseous and liquid phase mixtures.15,18 Magnetic activated carbons are composite materials that consist of activated carbon and magnetic labels, including magnetite (Fe3O4) and maghemite (γ-Fe2O3).15,19 Magnetic activated carbon has been successfully employed for the MSPE of various analytes such as bisphenol A,15 tartrazine,20 phenylurea herbicides21 and parabens.22
In this work, a micro–meso porous activated carbon/Fe3O4 (Bm) nanocomposite was prepared from the active charcoal precursor BAX-1500 and investigated for the magnetic solid-phase extraction of caffeine prior to their determination by gas chromatography-mass spectrometry. The main experimental parameters that influence the adsorption and desorption steps were optimized and the developed method was validated. The adsorption mechanism of caffeine onto the nanocomposite was evaluated. The novel sorbent was successfully applied, for the first time, for the MSPE of caffeine from surface water samples prior to its determination by GC-MS.
For the synthesis of the magnetite nanoparticles (Fe3O4), iron(III) chloride hexahydrate (FeCl3·6H2O), iron(II) chloride tetrahydrate (FeCl2·4H2O) and ammonia solution (NH3) were purchased from Sigma-Aldrich. All chemicals used during the synthesis of the sorbent were of reagent grade. Wood-based activated carbon (BAX-1500) was manufactured by Mead Westvaco (Richmond, Virginia, USA). River and lake surface water samples were collected in Vienna (Austria) and filtered with nylon filter membranes, pore size 0.45 μm, prior to the MSPE procedure.
For the preparation of the magnetite-impregnated activated carbon, the wood-based activated carbon, BAX-1500 (B)15 was initially washed in a Soxhlet apparatus to remove soluble impurities. Then, half a gram of the material was dispersed in 150 mL water under ultrasonic irradiation for 30 min, until a homogenous suspension was obtained. Subsequently, magnetite (0.25 g) was added and the mixture was sonicated for 30 min. Finally, the resulting magnetic micro–meso porous activated carbon was collected by a magnet and freeze–dried.
A Shimadzu GC-2010 Ultra gas chromatograph with quadrupole mass spectrometry (MS) detector (Shimadzu, Tokyo, Japan) was used for determination of caffeine. Helium (99.999%, Messer, Gumpoldskirchen, Austria) was used as the carrier gas at a constant volumetric flow rate of 1.5 mL min−1. The injector temperature was 280 °C, while ion source and interface temperatures were 250 °C and 200 °C, respectively. A DB-5-MS Ultra Inert column (25 m × 0.25 mm internal diameter, 0.25 μm film thickness) was used as stationary phase (Agilent, Santa Clara, CA, USA). The oven temperature program was as follows: initial temperature 100 °C, ramp to 200 °C at 45 °C min−1 (held for 7 min), ramp to 320 °C at 45 °C min−1 (held for 3 min). Injection of 2 μL of sample was performed with a split ratio of 1:10. Solvent delay was set at 4.0 min and the total run time was 14.9 min. The elution time of caffeine was 5.5 min and therefore the mass detection was stopped after 6.5 min. Caffeine was quantified in selected ion monitoring (SIM) mode recording m/z 194 as the target ion and m/z 109 for qualitative confirmation.
A VWR Ultrasonic bath was used for the ultra-sound assisted extraction (VWR International, Radnor, Pennsylvania, United States). Moreover, for the preparation of Bm a heating magnetic stirrer (RW 20 digital, IKA Labortechnik, Staufen, Germany) was employed.
Nitrogen adsorption–desorption isotherms for the raw and Bm activated carbon as well as for magnetite are presented in Fig. S1 (ESI†). From the isotherms it can be evaluated that B carbon can be considered as micro–meso-porous with a surface area of 2490 m2 g−1 and total pore volume of 1.619 cm3 g−1 while after magnetite impregnation, the surface area for Bm carbon decreases to 1559.8 m2 g−1 and the total pore volume to 1.170 cm3 g−1 mainly due to pore blocking effects as a result of magnetite deposition. Table S1 (ESI†) summarizes the textural parameters of Fe3O4, B and Bm. Pore size distributions curves (PSDs) are presented in Fig. S2† and reveal that after magnetite impregnation, a decrease in the pore volume for pores larger than 20 Å possibly occurred due to the deposition of magnetite in larger pores, as well as a slight increase in the volume of pores smaller than 10 Å possibly due to the formation of new pores attributed to the magnetite impregnation. The results indicate that activated carbon is a suitable adsorbent for caffeine with a molecular diameter of about 0.78 nm.
Moreover, Fig. 2 shows the FTIR spectra of the raw activated carbon, B, and of the magnetic carbon, Bm, as well as its counterpart after caffeine adsorption, providing information about their surface chemistry and the interactions of caffeine with the surface of magnetic activated carbon.
Fig. 2 FTIR spectra for caffeine (red), for the activated carbon sorbent B (green) and for Bm before (black) and after (blue) the adsorption of caffeine. |
The main characteristic absorption peaks of B sample could be assigned at 1700 cm−1 to the stretching vibration of CO in carboxyl groups, at 1630 cm−1 to the aromatic skeletal stretching (CC) vibration in aromatic rings, at 1460 cm−1 to vibrations of the C–C group and in the range of 1000–1300 cm−1 to the vibrations of the functional groups of –CO and –OH. For the magnetic Bm carbon, the band at 1700 cm−1 is assigned to the carboxyl CO stretching while the band at about 1620 cm−1 is the combination of CC stretching vibration of the aromatic ring structures and conjugated systems such as diketones, ketoesters, quinones. The bands at 1580 and 1400 cm−1 are assigned to the asymmetric and symmetric carboxylate units coordinated to the magnetite while the bands from ∼1300 cm−1 to ∼1000 cm−1 are assigned to C–O–C lactone structures, stretching C–O vibrations of phenol structures and ethers and bending O–H modes of phenol structures and at ∼900 cm−1 to epoxy groups.33 These bands presented a higher intensity indicating that surface oxygen groups would facilitate the attachment of magnetic nanoparticles through a covalent coupling or electrostatic interactions. The bands at 695.2 and 468.8 cm−1 correspond to the Fe–O bond vibration of impregnated Fe3O4 nanoparticles.34,35
The FTIR spectrum of magnetic activated carbon, after caffeine adsorption, also presented in Fig. 2, presents evidence about the adsorption of caffeine onto the carbon surface as well as about the adsorption mechanism. The spectrum of magnetic activated carbon, after caffeine adsorption presents a shift of the band due to CC stretching vibration of the aromatic ring structures, compared to pure magnetic carbon, from 1683 to 1607 cm−1, due to π–π electron donor–acceptor interaction, also known as π–π interaction. The interaction exists between the π electron-rich surface of magnetic carbon and the π electron cloud of the two aromatic rings of caffeine.36 Besides, the n–π electron–donor–acceptor interaction, also known as n–π interaction, which occurs between lone pair electron-rich atoms such as oxygen on the surface of carbon and π electron cloud of caffeine molecules as was also discussed in Tran et al.37 The broadening of peak intensity of CC, at 1657, as well as the band at 1053 cm−1 and the band at ∼1200 cm−1 due to C–N supports the assumption of caffeine adsorption on the surface of carbon.38 Besides, in the pH region between 4 and 10.4, caffeine exists in its cationic form and since all experiments were performed at pH ∼ 7, the carbon surface was negatively charged due to the predominance of the negatively charged carboxylate moieties. Electrostatic attraction could be also developed between the adsorbate and the adsorbent, indicating that the adsorption of caffeine on the magnetic carbon surface could be also be based on electrostatic interactions.39 Additionally, the appearance of C–N stretching vibration at ∼1200 cm−1 in the caffeine treated carbon demonstrated that the caffeine donated electrons to the carbon surface, while the intensity increase of the C–O absorption at ∼1053 cm−1 showed that the caffeine acted as an electron acceptor from the carbon. Thus, caffeine was also adsorbed on magnetic carbon surface via the electron donor–acceptor mechanism. The N atom attached in the five membered (imidazole) ring of caffeine can be considered as electron donor to the CO group attached to the carbon surface, whereas the CO group in the six membered (pyrimidine) ring of caffeine can act as electron acceptor.40,41 From FTIR results it is seen that caffeine can be successfully adsorbed on magnetic carbon's surface.
The SEM micrographs of Bm activated carbon, presented in Fig. S3,† show that the surface texture presents a spongy structure that exhibits defects and cavities possibly attributed to the impregnation of Fe3O4 nanoparticles. Moreover, no significant changes were observed on the material's surface, after the adsorption of caffeine.
In order to obtain the maximum extraction efficiency, sufficient adsorption time is required for the complete dispersion of the sorbent in the sample, as well as for effective mass transfer in order to reach the extraction equilibrium.2,3 Herein, adsorption time of 1, 5, 10, 15, 20, 25 and 30 min were evaluated. As shown in Fig. 3, the extraction efficiency increased from 1 to 10 min and no further increase was observed afterwards. Therefore, 10 min was chosen as the optimum adsorption time.
Fig. 3 Effect of adsorption time on the MSPE process. Normalization of peak area was performed by dividing the peak area for each value by the peak area at 1 min. |
Subsequently, the addition of NaCl was evaluated at different concentrations (0, 2.5, 5, 10, 20 and 30% w/v). The salting-out effect can enhance the extraction efficiency, by decreasing the solubility of organic analytes.3 This was also the case here at the lower of the investigated salt concentrations, since the addition of NaCl up to the concentration of 5% w/v enhanced the extraction efficiency of caffeine, as shown in Fig. 4. Then, the extraction efficiency remained constant until the concentration of 20% w/v. However, further increase in NaCl concentration led to a drastic decrease of extraction efficiency. This can be explained by the significant increase in viscosity of the solution at high slat concentrations, resulting in a hindrance of the adsorption of the target analytes by reducing the extraction efficiency and diffusion coefficient.3 This explanation is supported by data published for the dynamic viscosity η of aqueous NaCl solutions: for an aqueous solution of 5% w/v NaCl, η = 0.89 mPa.s and for 20% w/v NaCl, η = 1.12 mPa.s while for a 30% w/v NaCl solution this value increases to η = 1.57 mPa.s (data interpolated from Zhang and Han48). This represents a 40% increase in viscosity which may well explain the decrease of extraction efficiency of approximately the same order of magnitude. At the lower concentrations of NaCl, the increase in solvent viscosity is comparatively small, and more than compensated by the above-mentioned salting-out effect. Therefore, all further experiments were conducted with a salt addition of 5% w/v.
The key factor for the selection of the most appropriate elution solvent is polarity.42 For this reason, elution solvents of different polarities were evaluated. The studied elution solvents were acetonitrile (ACN), methanol (MeOH), toluene (TOL), dichloromethane (DCM) and a mixture of MeOH:ACN 50:50 v/v. As shown in Fig. 5, acetonitrile and the mixture of MeOH:ACN 50:50 v/v exhibited the strongest desorption power among the examined eluents. In order to avoid the need for solvent mixing, pure acetonitrile was chosen as elution solvent. Subsequently, different quantities of acetonitrile (100, 250, 500 and 1000 μL) were evaluated. Generally, the quantity of the elution solvent should be sufficient for the complete elution of the adsorbed analyte from the sorbent. It was found that 500 μL of acetonitrile was sufficient for the elution of caffeine from the micro–meso porous activated carbon/Fe3O4 nanocomposite.
Desorption time is another critical factor that should be carefully optimized in order to provide complete elution of the target analytes from the nanocomposite. For the evaluation of desorption time the following desorption time spans were studied: 1, 2.5 5, 10 and 15 min. As it can be observed in Fig. 6, one minute was enough to desorb the target analyte. However, for reproducibility reasons, a desorption time of 2.5 min was chosen.
Fig. 6 Effect of desorption time on the MSPE process. Normalization of peak area was performed by dividing the peak area for each value by the peak area of 1 min. |
Normalization of peak area was performed by dividing the peak area for each value by the peak area of DCM.
Validation parameter | Result |
---|---|
Calibration curve (y = peak area, x = ng L−1) | y = 2233.1.1x + 1067.7 |
R2 | 0.9997 |
Linear range (ng mL−1) | 0.60–12.5 |
LOD (ng mL−1) | 0.18 |
LOQ (ng mL−1) | 0.60 |
Extraction recovery (%) | 91.1 |
Enhancement factor | 36.4 |
Intra-day RSD% | 5.6 |
Inter-day RSD% | 6.2 |
Sorbent | Sample preparation technique | Detection system | Sorbent mass (mg) | Adsorption time (min) | Desorption time (min) | Relative standard deviation (%) | Linear range (ng mL−1) | LOD (ng mL−1) | Ref. |
---|---|---|---|---|---|---|---|---|---|
Graphene oxide | Ultra-sound assisted d-SPE | HPLC-UV | 15 | 15 | 5 | 1.8 (intra-day) 2.9 (inter-day) | (0.003–5) × 103 | 0.11 | 43 |
Octadecyl silica | On-line SPE | HPLC-UV | 100 | — | — | >12% (intra-day) | (15–200) × 10−3 | 0.01 | 44 |
3D-graphene | Ultra-sound assisted MSPE | GC-MS | 50 | 0.5 | 0.5 | 5.9 (intra-day) 7.1 (inter-day) | (0.5–500) × 103 | 100 | 45 |
Molecular sol–gel imprinted fiber | SPME | GC-MS | — | 60 | — | 10 (intra-day) 16 (inter-day) | (1–80) × 103 | 100 | 46 |
Molecularly imprinted polymer | SPE | ESI-IMS | 50 | >15 | >15 | <6 | (0.5–20.00) × 103 | 200 | 47 |
Bm | Ultra-sound assisted MSPE | GC-MS | 2.5 | 10 | 2.5 | 5.6 (intra-day) 6.2 (inter-day) | 0.60–12.5 | 0.18 | This work |
The RSD% of the proposed method was similar to those of ref. 45 and 47 and it can be considered as satisfactory, while it was better compared to that of the on-line SPE method (ref. 44). Finally, it should be noted that the LOD of this study was similar to the LOD value reported in ref. 43, higher that the LOD value reported in ref. 44, but lower than the LOD value of ref. 45–47.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra01564h |
This journal is © The Royal Society of Chemistry 2021 |