Renata A.
Grothe
a,
Alnilan
Lobato
a,
Bassim
Mounssef
Jr.
a,
Nikola
Tasić
a,
Ataualpa A. C.
Braga
a,
Adriano O.
Maldaner
b,
Leigh
Aldous
c,
Thiago R. L. C.
Paixão
*a and
Luís Moreira
Gonçalves
*a
aDepartamento de Química Fundamental, Instituto de Química, Universidade de São Paulo (USP), Avenida Prof. Lineu Prestes, 748, Cidade Universitária, São Paulo – SP, 05508-000, Brazil. E-mail: trlcp@iq.usp.br
bInstituto Nacional de Criminalística, Polícia Federal Brasileira (PFB), Q7, L23, Asa Sul, Brasília – DF, 70610-200, Brazil. E-mail: lmgoncalves@iq.usp.br
cDepartment of Chemistry, King's College of London, Britannia House, 7 Trinity Street, London, SE1 1DB, UK
First published on 12th January 2021
The analysis of ‘cutting’ or additive agents in cocaine, like benzocaine (BZC), allows police analysts to identify each component of the sample, thus obtaining information like the drugs’ provenience. This kind of drug profiling is of great value in tackling drug trafficking. Electropolymerized molecularly imprinted polymers (e-MIPs) on portable screen-printed carbon electrodes (SPCEs) were developed in this study for BZC determination. The MIPs’ electropolymerization was performed on a carbon surface using the anaesthetic BZC as the template molecule and 3-amino-4-hydroxybenzoic acid (3,4-AHBA) as the functional monomer. The build-up of this biomimetic sensor was carefully characterized by cyclic voltammetry (CV) and optimized. Cyclic voltammetric investigation demonstrated that BZC oxidation had a complex and pH-dependent mechanism, but at pH 7.4 a single, well-defined oxidation feature was observed. The BZC-MIP interactions were studied by computer-aided theoretical modeling by means of density functional theory (DFT) calculations. The electroanalytical methodology was effectively applied to artificial urine samples; BZC molecular recognition was achieved with a low limit of detection (LOD) of 2.9 nmol L−1 employing square-wave voltammetry (SWV). The e-MIPs were then used to ‘fingerprint’ genuine cocaine samples, assisted by principal component analysis (PCA), at the central forensic laboratory of the Brazilian Federal Police (BFP) with a portable potentiostat. This electroanalysis provided proof-of-concept that the drugs could be voltammetrically ‘fingerprinted’ using e-MIPs supported by chemometric analysis.
A literature survey demonstrated extremely few studies have reported on the electroanalysis of BZC (Table 1),3,13–15 in various types of samples. There is only one report on molecularly imprinted polymers (MIPs) for BZC quantification: Sun et al. developed molecularly imprinted microspheres via aqueous-suspension polymerization with methacrylic acid as the functional monomer. The microspheres were then used in a molecularly imprinted solid-phase extraction system to extract BZC in human serum and fish tissue, prior to BZC analysis and quantification by high-performance liquid chromatography with UV spectrophotometric detection (HPLC-UV).16 This means that, to the best of the authors‘ knowledge, so far electropolymerized MIPs (e-MIPs) have not been developed for BZC detection and quantification.
Electroanalytical technique | Electrode | LOD/μmol L−1 | LOQ/μmol L−1 | Matrix | Ref. |
---|---|---|---|---|---|
ABS – acetate buffer solution; BDDE – boron-doped diamond electrode; BRB – Britton–Robinson buffer; cap-b-MWCNT-BPPGE – capsaicin modified bamboo-like multiwalled carbon nanotube modified basal plane pyrolytic graphite electrode; CPE – carbon paste electrode; CV – cyclic voltammetry; DME – dropping mercury electrode; DPAdSV – differential pulse adsorptive stripping voltammetry; DPV – differential pulse voltammetry; Nf – nafion; p-CMCPE: p-chloranil modified carbon paste electrode; PBS – phosphate buffer solution; PT – polythiophene; PtE – platinum electrode; TiO2-GO/CPE – titanium dioxide – graphene oxide/carbon paste electrode. | |||||
SWV | GCE-MIP | 0.0029 | 0.0098 | Artificial urine | This work |
SPCE-MIP | 0.059 | 0.20 | PBS, pH 7.4 | ||
Bromatometry | Helical PtE | — | — | HCl, pH 1 | 91 |
SWV | BDDE | — | — | BRB, pH 1.6 | 84 |
Bromatometry | PtE | — | — | H2SO4, pH 1 | 92 |
DPAdSV | Nafion-GCE | 0.0024 | 0.0080 | BRB, pH 2 | 61 |
SWV | Cap-b-MWCNT-BPPGE | 2.5 | — | BRB, pH 1 | 93 |
p-CMCPE | 4.3 | ||||
DPV | Miniaturized BDDE | 0.08 | — | BRB, pH 4 | 13 |
SWV | 0.1 | ||||
Amperometry | CPE | 0.19 | — | BRB, pH 4 | 94 |
SWV | Graphite | — | — | HCL, pH 1 | 64 |
SWV | GCE, Pt | — | — | PBS, pH 6.8 | 95 |
CV | GCE, Pt, Au | — | — | PBS, pH 4 and pH 8 | 96 |
SWV | TiO2-GO/CPE | 0.25 | 0.83 | BRB, pH 2 | 14 |
Polarography | DME | 5.6 | 1.8 | PBS, pH 4 | 3 |
Amperometry | SPCE | 0.030 | 0.091 | PBS, pH 7 | 15 |
Amperometry | GCE | 0.06 | 0.30 | ABS, pH 4.8 | 97 |
CV | PT/GCE/Nf | 0.50 | — | PBS, pH 7 | 98 |
DPV | 0.05 |
MIPs have been used for a wide range of purposes and applications, from targeted drug delivery through to aiding chromatographic separations, purifications, and various means of sensing.9,17–24 Amongst the various synthetic routes for preparing MIPs, the synthetic electrochemical approach has emerged as advantageous due to the simplicity of preparation protocols, pronounced sensitivity, reproducibility of the molecularly-imprinted film, facile application, rapid analysis, low-cost, and resulting chemical and mechanical stability.4,23,25–27 Typically, an electropolymerized MIP (or e-MIP) is produced on the electrode surface by electropolymerization of functional monomer(s) in the presence of a template molecule; the latter is typically the desired analyte.23,28 Upon the formation of the polymer/template composite layer, the template is removed, and the resulting 3D architecture consists of a polymer with distributed pores which are complementary in size and shape to the analyte molecules. Such pores are prone to hosting and pre-concentrating the analyte, by chemical bonding or adsorption.99 Analytes pre-concentrated this way can be detected and quantified via various electrochemical techniques, such as cyclic voltammetry (CV), electrochemical impedance spectroscopy (EIS) or square-wave voltammetry (SWV).21,29–33 Research on e-MIPs has been fertile, these last years have seen improvements like the use of nanomaterials,34,35 recurring to computational studies to better understand polymerization and e-MIP–analyte interactions,23,28,36 the use of epitopes (a similar concept to dummy-MIP) for large molecules37 and bacteria,38 among other interesting developments.26,39–41
Police laboratories around the world mostly use chromatographic methodologies with various detectors for precise identification of BZC;42,43 spectrophotometric methodologies are used for an in situ approach, often using Raman44 or Infrared45 spectroscopy. In this work, the authors have developed an e-MIP sensing strategy based on the electropolymerization of 3-amino-4-hydroxybenzoic acid (3,4-AHBA) on a carbon surface in the presence of the BZC template. The goal was to demonstrate the proof-of-concept of applying an electroanalytical methodology – with its advantages of simplicity, low-cost, portability, and sensitivity – to identify BZC in biological fluids like urine and illicit samples. The latter is of extreme importance to support police forces gathering valuable data, such as seized drugs’ provenance. This identification helps identify cocaine routes, which is essential to coordinate intergovernmental response. For example, most cocaine arriving in Brazil is produced in Colombia, Peru and Bolivia,46 often passes through the Paraguayan border, then goes to North-American and European markets.47 While the e-MIP platform was successful for the selective quantification of BZC in synthetic urine, more complex results were obtained when analyzing genuine cocaine samples seized by the Brazilian Federal Police (BFP). The platform resolved multiple voltammetric features that addressed multiple adulterants and contaminants; when combined with principle component analysis (PCA) the e-MIP platform was able to discriminate various cocaine-based street samples swiftly. This is the first known application of voltammetry and MIPs in the discrimination analysis of genuine narcotics.
A scanning electron microscope (SEM, Model JEOL JSM-7401F, Japan) was employed to observe the surface structure of the MIP film on the SPCE. The SEM micrographs of the MIP film before and after use and the blank SPCE were observed at a magnification of 10000×. The acceleration voltage was 2 kV, working distance was kept at 8.0 mm, the sample chamber pressure was 9.53 × 10−5 Pa.
The e-MIP development process is demonstrated visually in Fig. 1. The electropolymerization in the monomer/analyte solution was performed by running 10 CV cycles in the potential range from 0 to +1.5 V (Fig. S2 in the ESI†). The solution was prepared by the dissolution of 3,4-AHBA in PBS at room temperature, followed by heat-assisted (65 °C) dissolution of BZC. The ratios between monomer and analyte in solutions were 1:3, 1:4, 1:5, 1:6, and 1:7, respectively, while the concentration of the functional monomer was kept at 0.5 mmol L−1. The non-imprinted polymer (NIP) sensor was prepared using the same polymerization conditions however without the template molecule. To remove the BZC after electropolymerization, the electrodes were subjected to 10 CV cycles in the potential range from −0.5 to +1.5 V in PBS with a scan rate of 200 mV s−1 (Fig. S3 in the ESI†).
Fig. 1 Schematics of the e-MIP development, adapted from literature.26 |
The functionality of the fabricated MIP sensor was additionally investigated by performing tests on synthetic human urine samples spiked with BZC (0.010–0.50 μmol L−1). Incubation was performed in urine samples diluted with PBS in the ratio of 1:10 for 30 minutes, followed by SWV detection of BZC. Recovery tests were performed on solutions with BZC concentrations of 0.02, 0.25, and 0.5 μmol L−1. Cocaine samples were diluted in PBS before analysis, no other sample pre-treatment was required.
All measurements were performed at room temperature (ca. 25 °C).
The data set was composed of 7 seized samples of cocaine hydrochloride and freebase originated from seizures performed by the BFP in different parts of Brazil in 2014. All samples were sent to the Forensic Chemistry Lab at the National Institute of Criminalistics in Brasília, to be analysed in the context of the PeQui Project.49 The samples’ composition is shown in Table S1 in the ESI.†
An initial study of 100 μmol L−1 BZC in PBS (pH 7.4, Fig. S4 in the ESI†) demonstrated one pronounced oxidation peak; no corresponding reduction feature was observed over the range of investigated scan rates (from 10 to 200 mV s−1). The peak currents (ip) were proportional to the square root of the scan rate, suggesting a diffusion-controlled process,65 with ip (in μA) = (5.3 ± 0.3)v0.5 (in V0.6s−0.5) − (0.25 ± 0.06), r2 = 0.993 (inlay of Fig. S4 in the ESI†).65 Moreover, the slope of the logarithm of the scan rate vs. the logarithm of peak current (0.43) is close to 0.5, which is expected for diffusion-limited systems.66–68
Next, the voltammetric oxidation of BZC was investigated in the pH range 1.0–12.0, using a universal buffer solution as supporting electrolyte (Fig. S5 in the ESI†). As can be observed in Fig. S5,† the single oxidation feature at pH 7 separated into two distinct oxidation processes from pH ≤ 5, whereas pH ≥ 11 a secondary, very significant oxidation process appeared. The latter observation is consistently with the reported electrochemical destruction of BZC at pH 12.2,63 whereas the former is consistent with more stable radical cation intermediates being reported pH < 7.62,64 Oxidation to a radical cation, followed by secondary oxidation of a dibenzocaine dimer62 at a higher potential is consistent with these observations. Conversely, the oxidation of R-NH2 to R-NO2 is also multistep process, passing through R-NHOH and R-NO intermediates,63 and this could explain the two features observed at pH ≤ 5. While further detailed analysis is required to identify the precise mechanism(s), the single oxidation peak observed at pH 7.4 PBS in Fig. S4† is suggested to correspond to an overlap of a number of distinct electrochemical and chemical processes. Nevertheless, since oxidation of BZC in PBS at 50 mV s−1 resulted in a well-defined, single oxidation peak, these conditions were taken forward for the direct electroanalytical quantification of BZC.
The overall process of the MIP sensor development was studied by way of CV (Fig. 2A) and EIS (Fig. 2B) after each fabrication step, using 2.0 mmol L−1 [(Fe(CN)6)]3− and 0.1 mol L−1 KCl solution as the test solution. The expected reversible voltammetric features of [(Fe(CN)6)]3−(ref. 65) were observed at the bare GCE. However, upon the formation of BZC-templated 3,4-AHBA-derived polymer layer (or MIP) on the GCE's surface, the current significantly decreased and the redox processes were completely removed. However, a non-imprinted polymer (NIP) layer achieved by polymerizing 3,4-AHBA in the absence of BZC retained much of the [(Fe(CN)6)]3− voltammetric features. Therefore, the NIP was non-electroactive whereas the MIP was completely insulating; it is not clear to authors why this occurs but one of the reasons may be the considerably lower thickness of NIP compared to MIP (as it will be showed subsequently); the presence of BZC therefore assists in the goal of forming a MIP, namely, to make it insulating relative to all molecules except the template. The potential non-innocent role of BZC in the film formation (e.g. beyond templating) does require further, more detailed investigation. Then, when incubating the MIP with 100 μmol L−1 BZC and scanning >+0.6 V resulted in the oxidation of BZC, indicating the MIP was successfully excluding non-specific molecules like [(Fe(CN)6)]3−, but displayed the desired voltammetric response to BZC. In the EIS analysis, the bare GCE displayed the expected lowest resistance when compared to the MIP after polymerization, after the template removal and after incubation.
The sensor fabrication protocol was subjected to a systematic optimization of its experimental variables, namely template concentration, number of the CV cycles, applied scan rate during the electropolymerization, and incubation time (Fig. S8 in the ESI†). The main criteria to pick the optimal conditions were the peak current's intensity obtained during the sensor testing by means of SWV after incubation with 30 μmol L−1 BZC in buffer, along with the resolution of the obtained signal. Initially, a template/functional monomer ratio study was performed, which showed the best signal was achieved by a high ratio of BZC, the 3,4-AHBA/BZC ratio of 1:6 was the optimum of all tested; 1:6 ratio was a considerably better than 1:5 and 1:7, and much better than 1:3 and 1:4. Similarly, a scan rate study showed that the optimal value was achieved in a very narrow range, with the best peak current value obtained for the sensor electropolymerized being 10 cycles at 50 mV s−1 (other scan rates tested were 10, 25, 75 and 100 mV s−1). The study on the number of cycles for electropolymerization demonstrated one of the main benefits of the proposed method, i.e. a drastic reduction of the average fabrication time in comparison to bulk or precipitation polymerization. As expected, the increase in the number of the cycles led to a significant increase in the peak currents up to 20 cycles (following the testing of 5 and 10 cycles), but a diminishing signal was observed after 20 cycles. For the sake of the experiment's overall time reduction, further analyses were performed only with 10 electropolymerization cycles, considering the already considerable high values of peak current obtained by 10 scans. Finally, an incubation time study was performed, which showed an exponential rise of the peak currents during incubation times from 5 to 15 minutes before reaching a signal saturation between 15- and 30-minute incubation time.
The production simulation consisted of 585000 steps run in an isothermic-isobaric ensemble, often called a NPT (constant Number of atoms, pressure and temperature) ensemble, after a 230000 steps thermalization. The first 30000 thermalization steps were made with rigid molecules, while in the subsequent 800000 steps only the water molecules were kept rigid. It was later considered the last 385000 steps for the survey of the pre-polymerization process. A box simulating the polymer–water interface, with the BZC molecule at the frontier between the systems – representing the interaction of the molecule with polymer cavities which would not entrap it after polymerization – was built using 1 BZC molecule, 489 3,4-AHBA molecules and 5079 water molecules. Configurations containing the first solvation shell were extracted from a total of 7700 configurations – one for each 50 simulation steps. It was observed that the first solvation shell contained a maximum of 6 3,4-AHBA monomers interacting directly with the BZC molecule, and from the total of 7700 configurations this was the case for 935 configurations. These were then chosen for a clustering analysis according to a hierarchical clustering method based on the unweighted pair group method with arithmetic mean (UPGMA),74 from which we obtained a total of 31 configurations clustered by a distance of 7.5 Angstroms in a distance matrix of the root-mean-square deviation (RMSD) of the atomic coordinates (all coordinates obtained are displayed as ESI†).
These 31 cavities had their geometry optimized using Grimme's GFN2-xTB method.75 This and all subsequent calculations were performed with the ORCA 4.0 package76,77 and the SMD implicit solvent model, with water as solvent.78 The total RMSD difference of the resulting cavities was then analysed and 10 cavities, within a maximum RMSD of 5.3 Angstroms from one another were finally chosen for a higher-level optimization and bond energy evaluation at the BP8679/def2-SVP80 level of theory and RI approximation81,82 and D3(BJ) dispersion. All of them had their minimum stationary points confirmed by frequency calculations (zero imaginary frequencies), which also provided the thermal corrections needed for the evaluation of their enthalpies. The real prevalence of these 10 cavities in the polymer was evaluated according to their formation energies, that is, the difference between the final enthalpy of the complex between BZC and six 3,4-AHBA monomers and the sum of the enthalpies of the same molecules as obtained by a relaxed optimization at the same level of theory. Only 2 of those cavities were found to have significant Boltzmann populations, being within a 1 kcal mol−1 difference from one another regarding their formation enthalpy in the presence of the BZC molecule. Those 2 cavities were finally tested against the procaine molecule by a relaxed optimization and the same level of theory. The images were produced with the VMD program83 and the results are shown in Fig. S9 in the ESI† and Fig. 3. Fig. S9† displays the 8 cavities that were not tested against the procaine molecule, to increase the formation energy, while Fig. 3 displays the two most stable cavities along with their procaine-bound counterparts. The most stable cavity, J-B (Fig. 3) has formation energy of 111.6 kcal mol−1, and is 0.7 kcal mol−1 stabler than cavity I-B. One would expect from these energy differences that cavity I would have less than a third of the cavity J population, and cavity J would dominate selectivity. One may observe that four types of interactions are present in the cavities: hydrogen bonding between the 3,4-AHBA monomers, hydrogen bonding between the monomers and the BZC's amine group π–π stacking between the monomers and the monomers and the BZC molecule. Formation enthalpy initially increases as the number of hydrogen bonds between the monomers increase. Cavities A-D show an increasing packing of the monomers around the BZC molecule along with the formation of multiple hydrogen bonds between 3,4-AHBA's hydroxyl, carboxyl and amine groups, leading to progressively increasing stability. As one may see, the most stable cavities in Fig. S9,† cavities F–H, show a common feature: two hydrogen bonds between the monomers’ and BZC's amine groups, and the alignment between the BZC's and 3,4-AHBA's aromatic systems, resulting in π–π stacking. In Fig. 3, the two most stable cavities differ in two aspects. Cavity J, the most stable, has three BZC-monomer hydrogen bonds, and BZC is part of a three-layer stacking with two other monomers, instead of just one as in cavity I. One may observe that the cavity J offers only slightly more stability to the procaine molecule than to the BZC, in agreement with the experimental trends. The procaine molecule shows a much larger affinity for the less abundant I cavity, which is less rigid and allows for better accommodation of the procaine's aromatic system, which must be distorted in the J cavity. One should further take notice of the cavities’ structural integrity. All the main interactions between monomers and the procaine's primary amine and aromatic groups and the monomers are maintained even with a thoroughly relaxed optimization with both BZC and procaine, strongly suggesting the cavities are real structural minima of the pre-polymerization complex.
According to theoretical simulation the driving force behind the MIP's selectivity appears then to be an arrangement of 3,4-AHBA monomers, bound between themselves by strong hydrogen bonds and also by π–π stacking, in such a manner that two interactions with BZC are maximized: hydrogen bonds to its amine group, and stacking with its aromatic system, which extends to the ester group. The best and most abundant cavity in these conditions would be J, which is slightly selective to procaine – procaine being 0.4 kcal mol−1 more stable in the cavity than BZC. Secondary cavities such as I, which have only two aromatic systems stacked and two hydrogen bonds with the amine group, have even stronger selectivity towards procaine, but much smaller populations in the pre-polymerization complex, and close selectivity to both BZC and procaine by the MIP as a whole will be dominated by energy differences in the dominant J cavity (Fig. 3). The combined Monte Carlo-Quantum Chemistry protocol is shown to be capable of accounting for the diversity of phenomena in the realistic MIP formation environment, and as such, for the rational design of MIPs for other targets, which are under investigation.
The selectivity of the optimized GCE-MIP device was then investigated, comparing BZC to seven structurally similar heterocyclic compounds, namely caffeine, phenacetin, levamisole, lidocaine, aminopyrine, procaine and hydroxyzine. It is worth mentioning that some of these compounds are also commonly used as the “cutting” additives in street-distributed drug samples, like BZC. For this purpose, 30 μmol L−1 solutions of each analyte in PBS were used, while the incubation time was kept at 45 minutes. This study's obtained results are presented in Table 2, including the so-called selectivity factor (α), which was calculated by dividing the BZC peak current by the interferent's peak current. Firstly, it can be observed that the peak potentials corresponding to the possible interferents vary when compared to the BZC peak potential. Additionally, based on α, only hydroxyzine and procaine could significantly compromise BZC analysis and yield a positive result. However, taking into consideration that their peak potentials are shifted towards different potentials than BZC, one should be able to differentiate their signal from a pure BZC signal. The similar affinity for BZC and hydroxyzine compounds is related to the main driving forces in the formation of the pre-polymerization complex: hydrogen bonding to the BZC's amine group and π–π stacking between BZC's aromatic system and the 3,4-AHBA monomers. In fact, hydroxyzine is the compound with the largest affinity for the polymer, and it has a chlorine replacing the amine group playing a double role: while it is able to also accept hydrogen bonds from the polymer, it is also able to direct electron density towards the aromatic system, contributing to its interaction with the stacked monomers. On the other hand, the aminopyrine molecule is the fourth with the largest affinity, just below BZC itself. It has no group analogue to BZC's amine but features a pyrazolone attached to the benzene ring that is able to interact with it by hyperconjugation, maintaining a planarity similar to the carboxyl-benzene system in BZC and thus also allowing for π–π stacking with the 3,4-AHBA monomers. It is interesting to note, and even analytically exploitable, that the compounds peaks’ potentials are different with the GCE-MIP that those obtained with a bare SPCE 2 or a boron-doped diamond electrode (BDDE).84 In particular, with the GCE-MIP it seems more possible to distinguish BZC (+0.92 V) from procaine (+0.97 V), whereas with the BDDE both had a peak potential of +1.1 V, and with the bare SPCE both had a peak potential of +0.9 V. Additionally, with the GCE-MIP lidocaine has a peak potential of +0.87, which with the SPCE would be difficult to differentiate.
The optimized GCE-MIP sensor was applied in the detection of BZC in spiked synthetic urine samples, with a concentration range from 0.010 to 0.50 μmol L−1 (Fig. S10 in the ESI†), resulting in an excellent linear relationship between BZC concentration and current, with r2 of 0.997. The analysis of BZC in urine can be of clinical relevance, including in cases of cocaine consumption.85 The limit of detection (LOD) and limit of quantification (LOQ) were calculated as three and ten times the standard deviation of the intercept/slope, respectively, giving a LOD of 2.9 nmol L−1 and LOQ of 9.8 nmol L−1. To the best of the authors’ knowledge this is the one of the lowest LODs reported for the electroanalytical quantification of BZC so far, only a work by Reddy and co-workers achieved the detection of a slightly lower concentration,61 as shown comparatively in Table 1.
Subsequently, to develop a portable e-MIP sensing platform for use in the swift profiling of drugs in the BFP's laboratory, the GCE was replaced with disposable screen-printed carbon electrodes (SPCE). The optimized conditions were then employed to form the MIP on the surface of these SPCE, which yielded similar voltammetric responses as observed on the GCE. The surface of the sensor was further characterized by scanning electron microscopy (SEM) (Fig. 5). Given the inherent roughness of the bare SPCE there were no observable differences between the MIP, NIP and the bare SPCE. This suggests that the formed polymeric film is very thin, which is consistent with the calculated film thicknesses of 77 ± 3 nm for the MIP and 33 ± 3 nm for the NIP. These film thicknesses were estimated according to the following equation:86,87
The SCPE-MIPs were next employed for analysis of 7 seized “cocaine” samples. These samples were known to include different quantities of BZC and cocaine (both from almost none to above 50% m m−1 concentrations), as well as several interferences used in the selectivity studies, such as phenacetin, caffeine, aminopyrine and lidocaine, and a range of unknown components (Table S1 in ESI†). SWV profiling of the 7 samples was achieved with the SPCE-MIPs using the samples dissolved in PBS (15 mg L−1). As can be seen in Fig. 6, each of the seven samples produced numerous distinguishable voltammetric signals; these numerous features prevented the voltammetric quantification of BZC or cocaine, though both their signal was detected. However, voltammetric fingerprinting of the various interferences indicated these were present in the SWV using the e-MIP.
Since the voltammetric information was a lot of data to be interpreted, PCA was used to evaluate the possibility, as a proof-of-concept, of discriminating the know contaminants in the cocaine samples. Hence, all the current values of the SWV recorded were used in this discrimination procedure. To obtain a better discrimination, it is normally used in the literature more than 70% of total variance explained (sum of percentage of information described in the PCs). Hence, the proposed work used 3 PCs to obtain 81.8%, indicating a large amount of original information described in the discrimination process. From Fig. 7 (the score plot of the proposed discrimination using PCA), it is possible to see that the location of the contaminants is in different regions of the 3D plots. BZC is separated in the positive quadrant of the PC1 and PC2 and distinguished from procaine using the PC3 information. Additionally, the aminopyrine is the only adulterant in the PC2 positive region and PC1 negative region. The hydroxyzine is the only contaminant in the negative area of the PC1 positive and PC2 negative quadrant. Lidocaine, levamisole, caffeine, and phenacetin reported in the PC1 negative – PC2 negative quadrant and PC3 component discriminated caffeine and phenacetin from lidocaine levamisole. The discrimination between these two groups, lidocaine and levamisole and caffeine and phenacetin, could be more complicated than voltammetric behaviour. Still, some dual detection devices could be used to add more information to the discrimination process.89 Hence, the result demonstrates proof-of-concept that SPCE-MIP SWV could be employed as a rapid forensic fingerprinting analysis of narcotics.
Fig. 7 PCA score plot obtained from the SWV current values extracted from each electrochemical experiment performed for each contaminant. |
The last Scientific Working Group for the Analysis of Seized Drugs (SWGDRUG) recommendations90 divide the analytical methods for drugs into 3 categories with different levels of selectivity: A – “Selectivity through structural Information” (e.g. mass spectrometry); B – “selectivity through chemical and physical characteristics” (e.g. UV-Vis spectroscopy); and C – “selectivity through general or class information” (e.g. spot tests). Then, two combinations of techniques are accepted as the minimum suitable identification, using (1) A+(A or B or C), and (2) B+B+(B or C). At the moment, electrochemical techniques are not part of the options. The authors advocate that a properly validated electroanalytical methodology should be included in the category B, since it can provide specific electrochemical information to identify forensic analytes; the results presented here represent a significant step in this direction.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0an02274h |
This journal is © The Royal Society of Chemistry 2021 |