Sabrein H. Mohamed*a,
Alyaa I. Magdyb and
Ashour A. Ahmedc
aChemistry Department, Faculty of Science, Cairo University, Giza, Egypt. E-mail: sabrein@sci.cu.edu.eg; sabrein_harbi@yahoo.com
bChemistry Department, Faculty of Engineering, Madina High Institute for Engineering and Technology, Giza, Egypt
cInstitute of Physics, University of Rostock, D-18059 Rostock, Germany
First published on 15th August 2018
Clopidogrel is an oral, thienopyridine class antiplatelet agent used to inhibit blood clots in coronary arteries, peripheral vascular and cerebrovascular diseases. A spectrophotometric method was developed for clopidogrel bisulfate (CLOP·H2SO4) determination using bromocresol green (BCG) as an ion-pairing agent. To explore the binding nature of CLOP·H2SO4 with BCG at a molecular level, quantum chemical calculations have been performed. DFT based full geometry optimization has been carried out for BCG and clopidogrel in basic (CLOP) and protonated (CLOP+) forms as well as for BCG ion-pairs with CLOP and CLOP·H2SO4. The DFT calculations referred to the stability of the BCG–CLOP+ ion-pair and its spontaneous formation reaction from BCG and CLOP·H2SO4 compared to the BCG–CLOP-ion-pair. Furthermore, the UV-visible spectra and their corresponding excited states and electronic transitions for BCG, BCG–CLOP+ ion-pair, and BCG–CLOP ion-pair have been investigated. These spectra provided a molecular level understanding of the nature of the different intra-molecular and intermolecular electronic transitions in the BCG ion-pairs with CLOP+. Moreover, the quantitative analysis based on extracting a yellow-formed ion-pair into chloroform from aqueous medium was carried out. The ion-pair exhibits an absorption maximum at 413 nm. The optimum conditions of the reactions were studied experimentally and optimized. The calibration graph shows that CLOP·H2SO4 can be determined up to 100.0 μg mL−1 with detection limit (LOD) of 0.57 μg mL−1 and quantification limit (LOQ) of 1.86 μg mL−1. The low relative standard deviation values, 0.16–1.16, indicate good precision. The results were compared to other published data and were treated statistically using F and t-tests.
A review about the bioanalytical methods, pharmacokinetics and pharmacodynamics has been published regarding the update on the recent trends in drug interaction studies.4 The literature survey revealed that several analytical techniques have been reported for clopidogrel, where there is no previous study about its action with sulfonephthalein dyes. It was observed that there was a UV spectrophotometric method for its analysis in presence of its alkaline degredates5 and in its pharmaceutical formulation.6 Three visible spectrophotometric methods7 have been reported for its quantification in pure and pharmaceutical dosage forms based on the formation of ion-pair complexes of the drug with acidic dye Solochrome black T, oxidation of the drug with phenanthroline and oxidation with potassium permanganate, Table 1.
Reagent | Linear range μg mL−1 | LOD μg mL−1 | Slope, a L g−1 cm−1 | r2 | ε L mol−1 cm−1 | RSD% | λmax nm | Ref. |
---|---|---|---|---|---|---|---|---|
a r2: correlation coefficient, ε: molar absorptivity, RSD%: relative standard deviation, C.S: current study, BCG: Bromocresol green, SBT: Solochrome black T, PTL: phenanthroline. | ||||||||
BCG | Up to 100.0 | 0.57 | 1.00 × 10−2 | 0.9946 | 5.67 × 103 | 0.31–0.96 | 415 | C.S |
Direct UV | 40.0–70.0 | 0.40 | 1.00 | 1.0000 | 3.20 × 102 | — | 222 | 6 |
SBT | 15.0–25.0 | — | 1.87 × 10−1 | 0.9969 | 5.0781 × 104 | 0.69 | 510 | 7 |
(Fe(III)/PTL) | 10.0–50.0 | — | 7 × 10−3 | 0.9980 | 3.873 × 103 | 0.66 | 515 | 7 |
KMnO4 | 2.5–12.5 | — | 2.00 × 10−3 | 0.9980 | 21.27 × 103 | 1.56 | 410 | 7 |
Sulfonephthalein dyes are commonly used as indicators in acid–base titrations. They have been also used to build pH-sensors8 and for the spectrophotometric determination of different drugs.9,10 Correlation between the pKa of these dyes with the nature of the substituent group was studied using the stability quotients from absorbance data.11 The electron-donor group increases their pKa values and the electron-attracting group decreases these values. Spectrophotometry has an inherent simplicity, a low cost and a wide availability in most quality control laboratories, so it considered as the most convenient analytical techniques.
Based on the wide use of sulfonephthalein dyes, the main goal of the present study is to perform density functional theory (DFT) based molecular modelling to investigate the binding nature of clopidogrel in basic (CLOP) and protonated (CLOP+) forms with bromocresol green (BCG) at a molecular level. In addition, the use of BCG, Scheme 2, in the determination of the antiplatelet drug CLOP·H2SO4 as a way to get its concentration with a new simple, accurate and sensitive technique in its raw material and pharmaceutical formulations in comparison with the previously published literary.
The stoichiometric ratios were determined utilizing Job's method of continuous variation.12 Diverse volumes of 1.0 mmol L−1 CLOP·H2SO4 were treated with the corresponding complementary volume of 1.0 mmol L−1 BCG to give a total volume of 3.0 mL of both reagent and drug. Then the experiment was continued as mentioned above.
A more detailed examination for the ion-pair (1:1) and (1:2), drug to reagent, was continued by using Benesi–Hildebrand method.13 It was conducted by using variable concentrations of 0.2–1.2 of 0.5 mmol L−1 BCG, to which 1.0 mL 5.0 mmol L−1 CLOP·H2SO4 was added. Then the experiment was continued as mentioned above.
Fig. 1 Optimized geometries of CLOP, CLOP+, BCG, BCG–CLOP ion-pair, and BCG–CLOP+ ion-pair at the B3LYP/6-31+G(d,p) + Lanl2dz level of theory. |
For the ion-pair formation reaction, 1 BCG + 1 CLOP(CLOP+) → 1 BCG–CLOP(CLOP+) ion-pair, the binding energy (EB) between BCG and CLOP or between BCG and CLOP+ is calculated as follows:
EB = EBCG−CLOP(CLOP+)ion-pair − (EBCG + ECLOP(CLOP+)) | (1) |
EB | EZPE+thermalB | ΔHB | ΔGB | |
---|---|---|---|---|
(kcal mol−1) | ||||
BCG–CLOP | −9.90 | −8.69 | −9.28 | +1.88 |
BCG–CLOP+ | −19.49 | −17.74 | −18.33 | −8.90 |
Next, the UV-visible spectra for BCG and its ion-pairs with CLOP and CLOP+ were calculated theoretically (Fig. 2) for further understanding for the nature of the intra-molecular and inter-molecular interaction in BCG, BCG–CLOP ion-pair, and BCG–CLOP+ ion-pair. Regardless the shift in λmax between the experimental and theoretical UV-visible spectra, Fig. 2 provides two evidence points for the stronger interaction between BCG and CLOP+ compared to that between BCG and CLOP. First, the intensity or absorbance at λmax for the BCG–CLOP+ ion-pair is almost 63 times of that for the BCG–CLOP ion-pair. Second, the shift in λmax between the BCG and BCG–CLOP spectra is larger than that between the BCG and BCG–CLOP+ spectra. For more details, the possible excited states and the corresponding electronic transitions for BCG and its ion-pairs with CLOP and CLOP+ will be discussed briefly below.
For BCG, the calculated UV-visible spectrum showed excited states at wavelength range from 256.0 to 287.2 nm. The intensity of these states has been increased in the order 277.6 < 256.0 <269.1 < 269.8 < 257.9 < 287.2 < 261.4 < 262.3 < 285.1 < 270.7 < 280.0 < 265.5 nm. The most intense excited state at 265.5 nm consists of several electronic transitions involving HOMO−3 → LUMO+2 (16.3%), HOMO−1 → LUMO+1 (14.4%), HOMO−3 → LUMO+1 (14.2%), HOMO−1 → LUMO+2 (13.7%), HOMO−2 → LUMO+2 (6.8%), HOMO−3 → LUMO (6.5%), and HOMO−1 → LUMO+5 (6.2%). Focusing on the frontier molecular orbitals in Fig. 3, this explains that the most intense excited state involved the π → π* and π → σ* electronic transitions. These electronic transitions take place from the BCG benzene rings “A” and “B” to benzene ring “C” as well as to the Br atoms involved in the benzene rings “A” and “B”. The excited state at 280.0 nm occurred due to combination of HOMO → LUMO+1 (48.5%), HOMO → LUMO+5 (12.1%), HOMO → LUMO+2 (8.4%), and HOMO → LUMO+4 (7.6%) electronic transitions. Like the previous excited state, this state involved π → π* and π → σ* electronic transitions as well. Here, these electronic transitions happen from the benzene ring “A” to the benzene rings “B”and “C” and also to the C–Br bonds in the benzene rings “A” and “B”. At 270.7 nm, combination of the electronic transitions HOMO → LUMO+4 (15.8%), HOMO → LUMO+1 (15.2%), HOMO−2 → LUMO (14.1%), HOMO → LUMO+3 (13.1%), HOMO → LUMO+2 (6.0%), and HOMO → LUMO (5.0%) has been observed. This means that this excitation state involved π → π* and π → σ* electronic transitions from the benzene ring “A” to the benzene rings “A”, “B”and “C” and to the C–Br bonds. Furthermore, the electronic transitions HOMO → LUMO (69.3%), HOMO−1 → LUMO (8.5%), and HOMO−1 → LUMO+1 (5.3%) have been observed at 285.1 nm that are related to π → π* transitions from the benzene rings “A” and “B” to the benzene ring “C”. While π → π* electronic transitions have been observed at 262.3 nm from the benzene ring “A” to the benzene ring “C” through the HOMO−2 → LUMO (47.6%) and HOMO−2 → LUMO+1 (39.9%) transitions. For the rest of the excited states, only the most contributed electronic transition for every excited state will be mentioned briefly. Here, the electronic transitions HOMO → LUMO+2 (256.0 nm), HOMO−1 → LUMO+3 (261.4 nm), HOMO−1 → LUMO+1 (269.8 and 287.2 nm), HOMO−1 → LUMO (277.6 nm), HOMO−2 → LUMO+5 (257.9 nm), and HOMO−2 → LUMO (269.1 nm) have been observed at the corresponding wavelength (given in parentheses). These are related to electronic transitions from π of the benzene rings “A” and “B” to π* of the benzene rings “A”, “B”, and “C” and σ* of C–Br bonds. The last exited sates can summarize all the possible electronic transitions that take place in BCG.
For the BCG–CLOP+ ion-pair, the intensity of the most intense excited states has the order 291.7 > 288.0 > 309.7 > 284.8 > 305.8 > 285.5 nm. For the excited state at 291.7 nm, the main electronic transitions are HOMO → LUMO+3 (72.8%) and HOMO−2 → LUMO+1 (18.6%) transitions. At 288.0 nm, the HOMO−2 → LUMO (44.2%), HOMO−2 → LUMO+1 (33.6%) electronic excitations have been observed while at 309.7 nm the HOMO → LUMO+1 (68%) and HOMO → LUMO (30%) transitions were the most abundant electronic transitions. For the excited state at 284.8 nm, the HOMO−1 → LUMO+3 electronic transition was the main transition. Eventually, the electronic transitions HOMO → LUMO, HOMO → LUMO+1, HOMO−1 → LUMO, HOMO−1 → LUMO+3, HOMO−2 → LUMO, and HOMO−2 → LUMO+1 have been observed at 305.8 and 285.5 nm. All these intense transitions can be simply classified into intra-molecular as well as intermolecular π → π* electronic transitions (Fig. 4). Specifically, the intra-molecular transitions take place from the BCG benzene rings “A” and “B” to the BCG benzene ring “C”. On the other hand, the intermolecular electronic transitions take place from the BCG benzene rings “A” and “B” to the clopidogrel benzene ring. The latter transitions can strengthen the interaction between BCG and clopidogrel in the BCG–CLOP+ ion-pair. Moreover, low intense excited states are observed at 303.6, 297.4, 279.6, 279.3, and 277.7 nm due to the electronic transitions HOMO → LUMO, HOMO → LUMO+2, HOMO−1 → LUMO, HOMO−1 → LUMO+1, HOMO−1 → LUMO+2, HOMO−3 → LUMO, and HOMO−4 → LUMO (Fig. 4). These excited states involved mainly intermolecular π → π* electronic transitions from the BCG benzene rings “A” and “B” to the clopidogrel benzene ring in addition to one intramolecular π → π* electronic transition from the BCG benzene ring “A” to the BCG benzene ring “C”. Furthermore, the HOMO−4 → LUMO transition is related to intramolecular π → π* electronic transition in clopidogrel from the thiophene ring to benzene one.
For the BCG–CLOP ion-pair, very low intense excited states are observed at 360.8, 355.1, 347.4, 341.3, 322.5, and 304.0 nm. These excited states involved the electronic transitions from HOMO to LUMO, LUMO+1, LUMO+2, and LUMO+3; from HOMO−1 to LUMO, LUMO+1, and LUMO+2; and from HOMO−2 to LUMO (Fig. 5). Excited states of intermediate intensity have been observed at 298.7, 313.3, 313.8, and 304.5 nm. Mainly these excited states have been arisen due to transitions from HOMO to LUMO+2, LUMO+3, LUMO+4, and LUMO+5; and from HOMO−1 to LUMO+2, LUMO+3, and LUMO+4. The most intense excited states, at 303.6 and 306.22 nm, have been explored via the electronic transitions HOMO → LUMO+4, HOMO → LUMO+7; HOMO−1 → LUMO+4, and HOMO−1 → LUMO+7. This means that the most abundant excited states included intramolecular and intermolecular π → π* electronic transition from the BCG benzene rings “A” and “B” to the BCG benzene ring “A” and the clopidogrel benzene ring. In addition, a π → σ* intra-molecular electronic transition has been observed to the C–Br bonds. Eventually, the UV-visible electronic transitions show that this BCG–CLOP ion-pair is weaker than the BCG–CLOP+ ion-pair although it shows intermolecular electronic transitions from BCG to clopidogrel. This is due to the intensity of the electronic transitions in the BCG–CLOP ion-pair is very small compared to that in the BCG–CLOP+ion-pair. This conclusion comes in a good agreement with the calculated binding (free) energies for both ion-pairs.
Finally, the effect of chloroform as a solvent on the calculated UV-visible spectra for BCG and its ion-pairs with CLOP and CLOP+ (see Fig. 2) has been introduced into Fig. 6. Here, the differences and similarities between the UV-visible spectra in vacuum and in chloroform will be discussed briefly. All the calculated UV-visible spectra in chloroform shifted to shorter wavelength compared to the spectra in the vacuum case. This is due to lower band gaps in vacuum (band gap: 0.181 a.u. for BCG, 0.160 for BCG–CLOP+ ion-pair, 0.140 for BCG–CLOP ion-pair) than in chloroform (band gap: 0.186 for BCG, 0.181 for BCG–CLOP+ ion-pair, 0.159 for BCG–CLOP ion-pair). Moreover, the shift in λmax between BCG and BCG–CLOP+ ion-pair is smaller in chloroform than in vacuum. In addition, higher intensities have been observed for all spectra in chloroform compared to the vacuum cases. Regardless these differences, the order of intensities of λmax and the order of the shift in λmax between the spectra calculated in chloroform are the same as in the vacuum cases. Mainly, the shift in λmax between BCG–CLOP and BCG–CLOP+ ion-pairs is similar for the chloroform and vacuum cases. Moreover, the possible excited states and the corresponding electronic transitions are almost similar for both vacuum and chloroform cases (for more details see Fig. S1–S3 and Tables S1–S3 in the ESI†).
Fig. 6 Calculated UV-visible spectra for BCG and its ion-pairs with CLOP and CLOP+ at the B3LYP/6-31+G(d,p) + Lanl2dz level of theory and using CPCM. |
Fig. 7 Absorption spectrum of 1.0 mmol L−1 CLOP·H2SO4 with 1.0 mmol L−1 BCG against a blank and 1.0 mmol L−1 BCG against chloroform as a blank. |
The effect of time on the formation of the reaction product at (25 ± 2 °C) was investigated by allowing the reaction to proceed at different times. The results revealed that the reaction was completed within 2 min. The absorbance remains stable for 24 h. This allowed the processing of large number of samples. Moreover, this increases the reliability of the methods as well as made it applicable for large number of samples.
Under the optimum conditions, the stoichiometry of the reaction between CLOP·H2SO4 and BCG was investigated by Job's method.9 The bell shape of Job's plot indicated that ion-pair formation between CLOP·H2SO4 and BCG followed 1:1 and 1:2 reaction stoichiometries, Fig. 8.
(2) |
The association constant of 1:1 and 1:2 ion-pairs was determined using Benesi–Hildebrand method applying the following equation.10
(3) |
Parameter | Value |
---|---|
a KADC is the association constant calculated applying Benesi–Hildebrand method. Kf is the formation constants calculated from the continuous variation data. | |
λmax (nm) | 413 |
Beer's law (μg mL−1) | Up to 100.0 |
Molar absorptivity (L mol−1 cm−1) | 5.67 × 103 |
Sandell sensitivity (μg cm−2) | 8.06 × 10−2 |
Ringbom range (μg mL−1) | 17.37–81.28 |
Limit of detection (LOD) (μg mL−1) | 0.57 |
Limit of quantification (LOQ) (μg mL−1) | 1.86 |
Slope (b)* (mL μg−1 cm−1) | 0.01 |
Intercept (a)* | 0.06 |
Correlation coefficient (r2) | 0.9946 |
Relative standard deviation (RSD) % (n = 3) | 0.31–0.96 |
KADC (L mol−1) | 5.34 × 103 |
εADλ (L mol−1 cm−1) | 2.43 × 103 |
Kf (n = 1) | 1.65 × 105 |
Kf (n = 2) | 7.56 × 1018 |
Conformity with calibration curve25 and Ringbom are evident in the concentration ranges up to 100.0 and 17.37–81.28 μg mL−1, respectively. The high molar absorptivity (5.67 × 103 L mol−1 cm−1) and the low Sandell sensitivity values (8.06 × 10−2 μg cm−2) reflect the good and high sensitivity of this method. The linearity of the calibration curve was approved by the high correlation coefficient (r2), 0.9946, and the small value of y-intercept (0.06) of the regression equation, Table 3.
LOD = 3s/k, LOQ = 10s/k | (4) |
The robustness of the method was evaluated by making small changes in some parameters as, the volume of dye, volume of extracting solvent and wavelength range. The effects of these changes were studied on the absorbance of the ion-pair. The changes had negligible influence on the results as revealed by small intermediate precision values expressed as % RSD (0.29–1.41%). Method ruggedness was demonstrated by carrying the analysis by two analysts, and also by a single analyst performing analysis using three different cuvettes. Intermediate precision values in both instances were in the range 0.58–1.63 indicating acceptable ruggedness.
Taken (μg mL−1) | aRecovery% ± SD | RSD% | t-Test | F-test |
---|---|---|---|---|
a Average of four replicates. | ||||
Plavix® tablets (75.0 mg CLOP·H2SO4/tablet) | ||||
23.99 | 98.00 ± 0.47 | 0.48 | 4.90 | 2.53 |
35.99 | 100.47 ± 0.51 | 0.51 | 0.47 | 2.36 |
59.99 | 99.89 ± 0.56 | 0.56 | 0.39 | 2.13 |
Borgavix® tablets (75.0 mg CLOP·H2SO4/tablet) | ||||
23.99 | 98.57 ± 0.76 | 0.77 | 2.65 | 1.55 |
35.99 | 100.13 ± 0.57 | 0.57 | 0.49 | 1.16 |
59.99 | 100.42 ± 0.69 | 0.69 | 0.08 | 1.42 |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c8ra05187a |
This journal is © The Royal Society of Chemistry 2018 |