key: cord-0888629-7rg80caq
authors: Szlósarczyk, Marek; Piech, Robert; Milc, Anna; Hubicka, Urszula
title: Fast and Sensitive Voltammetric Method for the Determination of Rifampicin on Renewable Amalgam Film Electrode
date: 2021-08-28
journal: Sensors (Basel)
DOI: 10.3390/s21175792
sha: 5b79543f374def13588d306caa5149d4183df48f
doc_id: 888629
cord_uid: 7rg80caq

In this work, a new sensitive voltammetric method for the determination of rifampicin without time-consuming preconcentration is presented. The objective was to develop a simple, fast and sensitive voltammetric procedure for the analysis of rifampicin in pharmaceutical products. The cyclic renewable mercury film silver-based electrode (Hg(Ag)FE) was applied as a working electrode for this purpose. The optimal conditions for the determination of rifampicin were defined, in terms of the composition of supporting electrolyte (including pH) and instrumental parameters (potential and time of deposition, step potential, pulse height). The method was validated resulting in a satisfactory linearity range of 0.4–250.0 µgmL(−1); the limits of detection and quantification are 0.12 µgmL(−1) and 0.4 µgmL(−1), respectively; and the repeatability of the method expressed as RSD is 4.1% (n = 6) with a surface area of 10.9 mm(2). The proposed method was successfully applied in the analysis of rifampicin in simple and composed pharmaceutical formulations.

Rifampicin (RIF) is a macrocyclic antibiotic, recommended as the first-line treatment of tuberculosis, also with other therapeutic agents [1] , in the prevention of the Neisseria meningitidis infection [2] and even for antibiotic prophylaxis of the postoperative endophthalmitis [3] . Considering reported variability of RIF pharmacokinetics, therapeutic ineffectiveness was explained by its low plasma concentrations [4, 5] . Problematic or delayed achievement of RIF therapeutic concentration may also contribute to the death of patients suffering from pulmonary tuberculosis. Moreover, several studies have shown a close relationship between RIF toxicity and its high plasma level [6] . Considering this variability of RIF, the therapeutic drug monitoring of RIF is helpful in tuberculosis therapy to prevent low plasma concentrations, drug-related toxicity, therapeutic failure and drug resistance or tuberculosis relapse [4, 5] .

Tuberculosis (TB) is one of the major life-threatening infectious diseases, millions of people continue to fall sick with TB each year. According to the WHO data, 10 million new cases of TB (including 1.2 million children) were reported, and 1.4 million people finally died from TB in 2019 [7] . Due to a considerable increasing rate of rifampicin resistance (RR) among strains of Mycobacterium tuberculosis (206k cases of multi-drug resistance MDR/RR-TB were detected and reported in 2019) combined with the evidence on the interaction between COVID-19 and TB in particular as public health implications (lower access to health services) [8, 9] . A recent WHO report on tuberculosis suggested urgent actions to improve coverage and quality of treatment for people with drug-resistant TB and better insight into MDR tuberculosis development. [7] . One of the factors which can help in this case is active ingredient analysis, necessary in drug quality control and as well as a useful tool in therapeutic drug monitoring during the treatment of tuberculosis [5] .

According to the available literature, the following analytical methods are commonly used for the determination of rifampicin in pharmaceuticals and body fluids: separation techniques-thin layer chromatography [10] with densitometric detection [11] or high-performance [12] , high-performance and ultra-high-performance liquid chromatography [13] , micellar electrokinetic chromatography [14] , capillary electrophoresis [15] and combined high-performance liquid chromatography-tandem mass spectrometry [16] ; optical techniques-spectrophotometry [17] and electroanalytical techniques. In the case of electroanalysis, stripping techniques are used preferably such as potentiometry and voltammetry [18] [19] [20] but in most cases voltammetry are limited to a positive potential range. The analysis in the negative potential range is possible using classical mercury electrode with high sensitivity, reproducibility and linearity range. However, the toxicity of mercury limits the application of the mercury electrodes in the analysis in both laboratory and portable applications [21] . One of the approaches to overcoming these limitations is to use a renewable silver amalgam film electrode (Hg(Ag)FE). A detailed description of the mentioned sensor and the first application was described previously [22] . The simple design of the Hg(Ag)FE electrode combined with the possibility of refreshing electrode surface provides a broad range of applications. Moreover, the use of the Hg(Ag)FE allows sensitive voltammetric determination of both inorganic and organic compounds, including active pharmaceutical ingredient (API) in various matrices [23] [24] [25] [26] [27] [28] [29] .

In this work, the application of cyclic renewable mercury film silver-based electrode (Hg(Ag)FE) in the determination of rifampicin is presented. The method based on differential pulse voltammetric technique was performed without preconcentration time allowing detection of rifampicin at trace level. The new method was examined with a successful application for the determination of rifampicin contents as API in several simple and composed pharmaceutical formulation.

All the voltammetric measurements were carried out at room temperature, using a multipurpose Electrochemical Analyzer M161 (MTM-ANKO, Kraków, Poland) controlled by PC. The typical three-electrode system of the electrode stand M164 (MTM-ANKO, Kraków, Poland) used Hg(Ag)FE as a working electrode, an Ag/AgCl reference electrode with a double junction and a platinum wire as an auxiliary electrode. SevenCompact pH meter S220 (Mettler-Toledo, Geneva, Switzerland) was used for pH measurements. Stirring was performed using a magnetic bar rotating with a speed of 500 rpm. For all the dataset processing and statistical calculations Statistica 13.3 (Tibco Software Inc., Palo Alto, CA, USA), OriginPro 2020 (OriginLab Corporation, Northampton, MA, USA) and MarvinSketch (ChemAxon, Budapest, Hungary) were used.

All reagents of analytical grade: CH 3 COOH (Suprapur), mercury GR for polarography, Triton X-100 and were from Merck (Darmstadt, Germany). A standard rifampicin solution of (10.3 mg/5 mL) and lower concentrations were prepared by dissolving rifampicin (Sigma-Aldrich, Steinheim, Germany) or by appropriate dilution in quadruple distilled water and were stored in a refrigerator. The silver wire (Ø 0.5 mm) for the film electrode was made of 99.99% polycrystalline silver (Goodfellow Science Park, Huntingdon, England). Before use, all glassware was immersed in a diluted (1:10) aqueous solution of HNO 3 (65%) and then rinsed copiously with distilled water.

Differential pulse voltammetry (DPV) was chosen for quantitative measurements of RIF using and the standard addition procedure. Before each measurement mercury film of Hg(Ag)FE electrode was refreshed and after conditioned applying a potential of −400 mV for 3 s. The potential of Hg(Ag)FE was changed in the following order: conditioning/starting potential −400 mV and recording in the cathodic direction from −400 mV to −1050 mV. The DPV instrumental parameters were as follows: step potential, 4 mV; pulse potential, 30 mV; time step potential, 20 ms (10 ms of waiting and sampling time) in 0.1 M CH 3 COOH as supporting electrolyte.

Ten tablets of Rifampicyna TZF ® and ten Rifamiazid ® (Polfa Tarchomin both) capsules content was weighed and powdered separately in an agate mortar, and the average weight of the tablet and capsule were calculated. Next, an appropriate amount of the powdered material was weighed and transferred to a volumetric flask and filled with quadruple distilled water to achieve the desired concentration. The obtained solution after 20 min of sonication, was filtered through a 0.45 µm membrane disk and filled up to the mark in the 10 mL volumetric flask. After, the obtained solution was ready to direct measurements, according to the proposed procedure, without additional pretreatment or extraction steps.

The effect of various supporting electrolytes on RIF peak was studied including the solutions of salts (potassium chloride and nitrate), base (sodium hydroxide), acid (acetic and phosphoric) and buffers (Britton-Robinson, phosphate, acetate). The height and shape of the peaks (based on the FWHM value-full width at half maximum) as well as the stability and repeatability of the signal were adopted as the evaluation criteria. In the investigated range, the pH influenced RIF peak current and potential causing its widening and enlarging. Although, the peak potential was shifted from −692 mV to −735 mV and the relationship with pH has a linear characteristic. In the case of RIF, the optimal pH ranged from 3.3 to 4.1, while outside these values its peak current was decreasing ( Figure 1 ). The best RIF peak shape, good signal-to-noise ratio (SNR) and optimal ionic medium conductivity were achieved for the solution of 0.1 M CH 3 COOH (pH = 3.3) and this concentration was chosen for further analysis. Considering the protonation of RIF, the optimal pH was close to the theoretical value calculated for these conditions at a given pH. Differential pulse voltammetry (DPV) was chosen for quantitative measurements of RIF using and the standard addition procedure. Before each measurement mercury film of Hg(Ag)FE electrode was refreshed and after conditioned applying a potential of −400 mV for 3 s. The potential of Hg(Ag)FE was changed in the following order: conditioning/starting potential −400 mV and recording in the cathodic direction from −400 mV to −1050 mV. The DPV instrumental parameters were as follows: step potential, 4 mV; pulse potential, 30 mV; time step potential, 20 ms (10 ms of waiting and sampling time) in 0.1 M CH3COOH as supporting electrolyte.

Ten tablets of Rifampicyna TZF ® and ten Rifamiazid ® (Polfa Tarchomin both) capsules content was weighed and powdered separately in an agate mortar, and the average weight of the tablet and capsule were calculated. Next, an appropriate amount of the powdered material was weighed and transferred to a volumetric flask and filled with quadruple distilled water to achieve the desired concentration. The obtained solution after 20 min of sonication, was filtered through a 0.45 µm membrane disk and filled up to the mark in the 10 mL volumetric flask. After, the obtained solution was ready to direct measurements, according to the proposed procedure, without additional pretreatment or extraction steps.

The effect of various supporting electrolytes on RIF peak was studied including the solutions of salts (potassium chloride and nitrate), base (sodium hydroxide), acid (acetic and phosphoric) and buffers (Britton-Robinson, phosphate, acetate). The height and shape of the peaks (based on the FWHM value-full width at half maximum) as well as the stability and repeatability of the signal were adopted as the evaluation criteria. In the investigated range, the pH influenced RIF peak current and potential causing its widening and enlarging. Although, the peak potential was shifted from −692 mV to −735 mV and the relationship with pH has a linear characteristic. In the case of RIF, the optimal pH ranged from 3.3 to 4.1, while outside these values its peak current was decreasing ( Figure  1 ). The best RIF peak shape, good signal-to-noise ratio (SNR) and optimal ionic medium conductivity were achieved for the solution of 0.1 M CH3COOH (pH = 3.3) and this concentration was chosen for further analysis. Considering the protonation of RIF, the optimal pH was close to the theoretical value calculated for these conditions at a given pH. 

Using the DPV technique RIF showed two peaks at potentials −693 mV and −966 mV in CH 3 COOH (pH = 3.3). The keys parameters of the DPV technique are pulse amplitude (dE), potential step amplitude (Es), waiting (tw) and sampling time (tp). So, the effect of the above instrumental parameters has been investigated for the first peak (twice as high as the second) in the ranges: 10-100 mV (both +/−) for dE, 1-9 mV for Es and 5-40 ms for both tw and tp. The increase of the pulse amplitude in negative mode caused peak shifting from −763 mV to −694 mV (Figure 2 ). The pulse amplitude above 40 mV caused a significant reduction of SNR due to the growth of background current and decrease of peak current (above 70 mV). At the optimal pulse amplitude of 30 mV, the RIF peak current was equal to 3.48 µA and showed the best SNR value.

Using the DPV technique RIF showed two peaks at potentials −693 mV and −966 mV in CH3COOH (pH = 3.3). The keys parameters of the DPV technique are pulse amplitude (dE), potential step amplitude (Es), waiting (tw) and sampling time (tp). So, the effect of the above instrumental parameters has been investigated for the first peak (twice as high as the second) in the ranges: 10-100 mV (both +/−) for dE, 1-9 mV for Es and 5-40 ms for both tw and tp. The increase of the pulse amplitude in negative mode caused peak shifting from −763 mV to −694 mV (Figure 2 ). The pulse amplitude above 40 mV caused a significant reduction of SNR due to the growth of background current and decrease of peak current (above 70 mV). At the optimal pulse amplitude of 30 mV, the RIF peak current was equal to 3.48 µA and showed the best SNR value. Considering SNR value, the best results were obtained for an amplitude of 30 mV, the selected pulse amplitude was applied for further studies. In the case of potential step amplitude, the rifampicin peak current showed significant growth up to 9 mV with significant growth of the background current ( Figure 3 ). Due to the limitation of measuring data by applying step potential above 4 mV this value was selected for further research. The range of waiting and sampling time were tested from 10 ms to 60 ms, and the best results were obtained with 10 ms for each of them. In order to reach the lowest RIF detection limit, two types of mercury electrodes were chosen for comparison. The voltammograms of RIF obtained on HMDE and Hg(Ag)FE were investigated, compared and showed in Figure 4 . The calculated current value of rifampicin peak, taking into account different surface areas of electrodes was 2.8 times higher for Hg(Ag)FE than for HMDE in the same condition. Considering SNR value, the best results were obtained for an amplitude of 30 mV, the selected pulse amplitude was applied for further studies. In the case of potential step amplitude, the rifampicin peak current showed significant growth up to 9 mV with significant growth of the background current ( Figure 3 ). Due to the limitation of measuring data by applying step potential above 4 mV this value was selected for further research. The range of waiting and sampling time were tested from 10 ms to 60 ms, and the best results were obtained with 10 ms for each of them. In order to reach the lowest RIF detection limit, two types of mercury electrodes were chosen for comparison. The voltammograms of RIF obtained on HMDE and Hg(Ag)FE were investigated, compared and showed in Figure 4 . The calculated current value of rifampicin peak, taking into account different surface areas of electrodes was 2.8 times higher for Hg(Ag)FE than for HMDE in the same condition. -1000 -900 -800 -700 -600 -500 -400 -300 -1000

-900 -800 -700 -600 -500 -400 -300 Figure 3 . Potential pulse step (Es) dependence on peak current for 1-9 mV. Instrumental parameters: ΔE = 30 mV, tw, tp = 10 ms. Stirring rate, 500 rpm. 

The solid electrode surface areas are usually greater than those of conventional mercury drop electrodes. However, when using the Hg(Ag)FE as a working electrode, its surface can be easily adjusted over a wide range. The rifampicin peak heights were linearly dependent on the surface area of the working electrode ( Figure 5 ). The linear relationship was described by following parameters: slope, 0.175 ± 0.004 [µA mm 

The solid electrode surface areas are usually greater than those of conventional mercury drop electrodes. However, when using the Hg(Ag)FE as a working electrode, its surface can be easily adjusted over a wide range. The rifampicin peak heights were linearly dependent on the surface area of the working electrode ( Figure 5 ). The linear relationship was described by following parameters: slope, 0.175 ± 0.004 [µA mm −2 ]; intercept, −0.240 ± 0.027 [µA] and Pearson correlation coefficient, r = 0.9996. The size of the working electrode of 10.9 mm 2 was selected for further studies. 

As a source of strong interferences in voltammetric methods, the surface-active compounds are usually suggested. Therefore, some common excipients found in pharmaceutical formulations (silicium oxide, carboxymethyl starch, sodium laureth sulfate, talc and magnesium stearate) and a nonionic surface-active compound (Triton X-100) were investigated. Based on the obtained results it was shown that tested excipients do not significantly affect RIF peaks. Whereas Triton X-100 solution caused reduce the signal by 47%, 80% and 87% for 0.5 mgL −1 , 1.2 mgL −1 and 2.5 mgL −1 , respectively ( Figure 6 ). Triton concentration above 1 mgL−1 causes peak drift to a more negative potential. It was suggested that hundreds of times concentration of surface-active compounds such as Triton X-100 

As a source of strong interferences in voltammetric methods, the surface-active compounds are usually suggested. Therefore, some common excipients found in pharmaceutical formulations (silicium oxide, carboxymethyl starch, sodium laureth sulfate, talc and magnesium stearate) and a nonionic surface-active compound (Triton X-100) were investigated. Based on the obtained results it was shown that tested excipients do not significantly affect RIF peaks. Whereas Triton X-100 solution caused reduce the signal by 47%, 80% and 87% for 0.5 mgL −1 , 1.2 mgL −1 and 2.5 mgL −1 , respectively ( Figure 6 ). Triton concentration above 1 mgL −1 causes peak drift to a more negative potential. It was suggested that hundreds of times concentration of surface-active compounds such as Triton X-100 does not significantly affect the quantitative analysis of RIF. The presence of isoniazid, as one of the components of Rifamazid ® was studied. Isoniazid in an acidified electrolyte solution (0.1 M CH 3 COOH) does not interfere and was studied before [28] .

As a source of strong interferences in voltammetric methods, the surface-active compounds are usually suggested. Therefore, some common excipients found in pharmaceutical formulations (silicium oxide, carboxymethyl starch, sodium laureth sulfate, talc and magnesium stearate) and a nonionic surface-active compound (Triton X-100) were investigated. Based on the obtained results it was shown that tested excipients do not significantly affect RIF peaks. Whereas Triton X-100 solution caused reduce the signal by 47%, 80% and 87% for 0.5 mgL −1 , 1.2 mgL −1 and 2.5 mgL −1 , respectively ( Figure 6 ). Triton concentration above 1 mgL−1 causes peak drift to a more negative potential. It was suggested that hundreds of times concentration of surface-active compounds such as Triton X-100 does not significantly affect the quantitative analysis of RIF. The presence of isoniazid, as one of the components of Rifamazid ® was studied. Isoniazid in an acidified electrolyte solution (0.1 M CH3COOH) does not interfere and was studied before [28] . 

The linearity range of up to 250 µgmL −1 was tested, but the smaller range was selected for further studies. The DP cathodic voltammograms of RIF for the 0.2-1.8 µgmL −1 concentration range without preconcentration step are presented in Figure 7 . In this concentration range the slope for regression line is 2.17 ± 0.05 [µAµg −1 mL] with correlation coefficient r = 0.996. The occurrence of the autocorrelation of residues was assessed using the Durbin-Watson test. In this case, the value of Durbin-Watson's statistics is d = 1.24, which is between the upper (du = 1.32) and bottom (dl = 0.82) threshold, so the test does not determine of correlation of the random component. Next, according to the method of Lagrange multipliers, the autocorrelation of the random component was not shown. The normal distribution of the residuals was examined by the Shapiro-Wilk test, (W = 0.964 > W*0.05 = 0.829; p = 0.84 > 0.05) and it was found that there are no bases for rejecting the hypothesis of a normal distribution of the random component. Therefore, heteroscedasticity of the random component was verified by Bartlett's test and the results are χ 2 = 0.009, df = 1, p = 0.92 > 0.05 which shown that variance of the residuals in the model is constant.

The estimation of the limits of detection (LOD) and quantification (LOQ) was based on SNR value of 3:1 and 10:1, respectively. Base on the obtained results of the short time analysis (without pre-concentration step), it is possible to achieve LOD = 0.12 µgmL −1 and LOQ = 0.4 µgmL −1 for RIF. The comparison of sensitivity obtained for RIF using other analytical techniques from available literature was shown in Table 1 . Obtained results are positioned within the best results using simple, low-cost instrumentation and short-time analysis. The repeatability of the method at a concentration level of the analyte as low as 10 µgmL −1 , expressed as RSD is 4.16% for six consecutive measurements. Bulk pharmaceutical samples (described in Section 2.4) and samples enriched with 75, 150 and 225 mg of RIF were used for the precision and recovery tests of the method. Quantitative analysis of the RIF samples carried out using the Hg(Ag)FE and the standard addition technique. The recovery of rifampicin in Rifamazid ranged from 98.1-102.9% and Table 2 . Results of rifampicin determination in pharmaceuticals formulation are presented in Table 3 . 

The presented DPV method for the electrochemical determination of rifampicin using a cylindrical silver-based mercury film electrode (Hg(Ag)FE), allows determining rifampicin at trace level, without preconcentration step. Determination of rifampicin under optimized condition exhibited high sensitivity (LOD = 0.12 µgmL −1 , LOQ = 0.40 µgmL −1 ), wide linearity range (0.2-250 µgmL −1 ), good precision (RSD = 4.3%), and good recovery. The repeatability of the method, with each measurement carried out at a fresh surface of the working electrode, is satisfactory and equals RSD = 4.16%. The proposed method is applicable for the rifampicin determination in pharmaceuticals. The obtained results were in good agreement with the content of API declared by the manufacturer, even in the presence of common excipients and isoniazid. The obtained results confirm that the developed method might be a useful tool for the quality control of pharmaceutical products and drug monitoring, whereas Hg(Ag)FE could be incorporated into portable voltammetric sensor systems. 

The data is available from the authors upon reasonable request.

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The study was financed as an R&D project by the Polish Ministry of Science of Education from research funds for the years 2015-2018 (KZDS/0005586).

Authors have declared no conflict of interest.