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Design and development of a multichannel potentiometer for monitoring an electrode array and its application in flow analysis

Design and development of a multichannel potentiometer for monitoring an electrode array and its... Instituto de Qu|mica, UNICAMP, CP 6154, CEP 13083-970, Campinas, è Brazil 2 CEQUP, Departamento de Qu|mica-F|èsica, Faculdade de Farmacia, Porto, è è Portugal A versatile potentiometer that works with electrode arrays in £ow injection and/or monosegmented £ow systems is described. The potentiometer is controlled by a microcomputer that allows individual, sequential multiplexed or random accesses to eight electrodes while employing only one reference electrode. The instrument was demonstrated by monitoring an array of seven £ow-through ion-selective electrodes for Ag‡ and for three electrodes for Cl¡ , Ca2‡ and K‡ . The ¢gures of merit of the individual and multiplexed (summed) readings of the electrode array were compared. The absolute standard deviation of the measurements made by summing the potential of two or more electrodes was maintained constant, thus improving the precision of the measurements. This result shows that an attempt to combine the signals of the electrodes to produce a more intense signal in the Hadamard strategy is feasible and accompanied by a proportional improvement in the precision of individual measurements. The preliminary tests suggest that the system can allow for 270 determinations per hour, with a linear range from 1:0 £ 10¡2 to 1:0 £ 10¡4 mol l¡1 for the three di¡erent analytes. Detection limits were estimated as 3 :1 £ 10¡5 , 3 :0 £ 10¡6 and 1:0 £ 10¡5 mol l¡1 for Cl¡ , Ca2‡ and K‡ , respectively. Introduction Potentiometric analytical methodologies have been widely employed for implementing online measurements owing to the ruggedness and selectivity of the sensors, which can be produced for many species of interest in the ® eld of agriculture [1], environmental chemistry [2] and clinical chemistry [3]. Ion-selective electrodes can be easily constructed, showing good analytical performance for the linear response range, selectivity, precision and lifetime. This kind of electrode is easy to miniaturize and can be arranged in arrays [4± 7]. The well-established ¯ ow techniques such as ¯ ow injection analysis (FIA) [8] and monosegmented ¯ ow analysis (MSFA) [9] can also be used for sample presentation and management (dilution and conditioning) in order to expand the useful concentration range and increase sample throughput. * To whom correspondence should be addressed. The goals of using an electrode array are to enhance the sensitivity and selectivity of the potentiometri c methodologies and/or to perform simultaneous determinations. Sensitivity can be improved by connecting the electrodes in series [10,11], which requires the use of several reference electrodes, even though a conventional monochannel potentiometer can be used. This approach is feasible only for determination of a single species, providing an increase in the slope of the analytical curve equivalent to the sum of the slopes of each electrode employed in the array. A simple alternative to double the sensitivity in ¯ ow injection potentiometry is achieved by placing two of the same ion-selective electrode in a single-line ¯ ow injection manifold where they work alternately as the reference electrode and the indicator electrode [4]. This approach provides an analytical signal similar to the pro® le of a second derivative of a potentiometric titration curve and the distance between the two electrodes should be optimized to obtain maximum sensitivity. The sensitivity of potentiometric measurements can also be improved by employing multichannel instruments [4,12]. The simplest version of this kind of potentiometer allows the electronic summing of the potential of a few electrodes (two or three) and employs only one reference electrode [4]. The capabilities of such potentiometers can be further expanded to allow simultaneous determinations if the electrodes of an array can be individually accessed. Furthermore, the instrument should be versatile to allow for summing up of the responses of more than one electrode and to perform any kind of readout from an individual reading to multiplexed readings, such as those necessary for the Hadamard multiplex approach [13± 15]. Most commercial potentiometers are monochannel instruments and access to the individual sensors of an electrode array cannot be made easily. Although recently some instrument manufacturers have oå ered multichannel instruments, the associated software is not suæ ciently ¯ exible to allow full user-tailored data acquisition [16]. Some contributions have been described in the literature for the development of multichannel potentiometers. Couto et al. [4] described a three-channel summing circuit for increasing the sensitivity of the potentiometric measurements, although the electrodes cannot be individually accessed. Alexander et al. [12] developed a multichannel circuit that can monitor up to six analytes simultaneously, but which employs a reference electrode for each indicator electrode. Forster and Diamond [6] used a four-channel potentiometer to perform non-linear calibration of ion-selective electrode arrays, where one of the electrodes should contain the ionophores of the three ISE. Although these contributions can either improve the sensitivity of the measurements [12] or perform simulta105 Journal of Automated Methods & Management in Chemistry ISSN 1463± 9246 print/ISSN 1464± 5068 online # 2002 Taylor & Francis Ltd http://www.tandf.co.uk/journals neous determinations [6], they do not provide random access to the electrodes or multiplexing reading, which is necessary for the Hadamard multiplexed approach. This paper describes a multichannel potentiometri c instrument, which is versatile to permit data acquisition in any user-selected form. The instrument has been evaluated for its ability to sum up the potential produced by many electrodes selective to the same analyte (Ag ‡ ) and to access the individual reading of an array containing three selective electrodes for Cl¡ , Ca2‡ and K ‡ . An evaluation of the instrument was made for operation with FIA and MSFA manifolds and for individual (sequential/random) or Hadamard multiplexed measurements. LM 348 + + + + + + + + ADG 201A To computer IE1 IE2 IE3 0.1 mF IE4 To A/D CA 3140 IE5 RE IE6 IE7 Materials and methods Reagents All reagents were of analytical grade and the solutions were prepared by using distilled and deionized water. The Ag‡ solutions in the 1:0 £ 10¡1 to 1:0 £ 10¡4 mol l¡1 concentration range were prepared by diluting a 1.0 mol l¡1 AgNO 3 stock solution. Solutions containing K‡ , Ca2‡ and Cl¡ ions in the 1:0 £ 10¡1 to 1:0 £ 10¡5 mol l¡1 concentration range were also prepared by proper dilution of 1.0 mol l¡1 KNO3 , Ca(NO3 )2 and NaCl stock solutions. The ionic strength of all solutions was adjusted to 1.0 mol l¡1 with a NaNO 3 solution. Multichannel potentiometer Figure 1 shows the electronic layout of the multichannel potentiometer constructed. The electronic circuit of the instrument is very simple and has been conceived to operate with up to eight selective electrodes and only one reference electrode. Each indicator electrode is connected to a high-impedance FET operational ampli® er (LM348) mounted in a buå er con® guration. The selection of the electrode (or electrodes) that will produce the signal is made through two four-input analogue switches (ADG 201A). The control of the switches is made by a computer interface (PCL-711S, Advantech), through eight digital outputs. The signal (or the sum of the signals if more than one electrode is simultaneousl y connected) is sent to the inverter input of a high-impedance operational ampli® er (CA3140). The reference electrode is connected to the non-inverter input of this operational ampli® er. When only one electrode is connected, the circuit works as a comparator. The same circuit acts as a summing point, adding the electrochemical potential diå erences generated by more than one electrode when they are simultaneously selected to participate in the measurement of a single species. Flow system Figure 2 shows a schematic diagram of the ¯ ow system employed. The system employs a four-channel peristaltic pump (Ismatec MS-Reglo) and a proportional injector IE8 Figure 1. Electronic circuit of the multichannel potentiometer. To computer OS RE C V Air A L L ISEA S I Figure 2. Schematic diagram of the £ow manifold. C, carrier £uid; P, peristaltic pump; V, three-way solenoid valve; L1/L2, air loops; A, sample loop; S, sample; OS, optical switch; ISEA, ion-selective electrode array; RE, reference electrode; W, waste. [17] to insert the sample into a MSFA or into a FIA (without the air loops, L1 and L2 ) manifold. An optoswitch (OS) is coupled to the sliding bar of the injector in order to ¯ ag each sample injection for the computer. The manifold includes a three-way solenoid valve (NResearch), placed before the proportional injector and used to deviate the carrier ¯ ow for stopped ¯ ow measurements. The electrode array was placed 10 cm from the injection port. The reference electrode was a standard double junction calomel (Corning Ð 900200), ® lled with a 1.0 mol l¡1 NaNO 3 external solution and placed after (at 1.0 cm) the electrode array. Tygon pumping tubes and polyethylene conducting tubes (0.8 mm i.d.) were employed throughout . The carrier solution was always a 1.0 mol l¡1 NaNO 3 solution. Electrode arrays Two electrode arrays were employed in the present study. The ® rst was used to investigate the performance of the potentiometer regarding its capability of adding the electrochemical potentials generated by each indicator electrode. The array contained seven silver sulphide ¯ ow-through electrodes with internal diameters of Potential (mV) 1.0 mm [18]. These 1.0 mm-thick electrode discs were arranged in series inside acrylic rods having a 15 mm external diameter and spaced from each other by 4.0 mm. The other array was built with three diå erent membrane-selective electrodes for K‡ , Ca2‡ and Cl¡ . The metal ion-selective electrodes were based on polymeric liquid membranes, constructed as described [19, 20], while the chloride-selective electrode was constituted by an AgCl/Ag2 S solid membrane [18]. This array was employed to evaluate the multiplexing and sequential reading capabilities of the potentiometer. Computer and software resources The multichannel potentiometer was controlled by an IBM-compatible 300 MHz PC-486 furnished with a PCL-711S (Advantech) parallel interface. This interface has a 12-bit analogue-to-digita l converter with a conversion rate of 100 kHz. Eight digital outputs of the interface were employed for electrode selection. Software written in Microsoft VisualBasic 5.0 was developed for electrode selection and acquisition, treatment and the storage of data. linear = - 2,57 slope = 400,6 r = 0,99994 3 4 5 6 7 number of electrodes Figure 3. Potential observed as a function of the number of silver electrodes used in the measurement for a 1:0 £ 10¡1 mol l¡1 Ag‡ solution. number and of which electrodes were selected to comprise the ® nal potentiometric signal. Figure 3 shows the signal as a function of the number of the electrodes that participate in the measurement; the straight line obtained presents a slope of 400.5 mV, very close to the sum (404.5 mV) of the individual slopes listed in table 1. This result also demonstrates that the electronic circuit of the multichannel potentiometer does not distort the signal when the electrical potentials of the indicator electrodes are summed, in accordance to the results obtained by Couto et al. [4] for summing two electrodes. In addition, the linearity of the response as a function of the concentration of Ag‡ ions is maintained from 10¡4 up to 10¡1 mol l¡1 , with a regression coeæ cient of 0.9996. Evaluation of the potentiometer with the K‡ , Ca2‡ and Cl¡ electrode array This array was evaluated for use with FIA and MSFA systems. In this case, the sampling rate of the signals produced by the diå erent indicator electrodes must be high enough to allow the sequential monitoring of the sensors. The sampling rate was determined by the time necessary for the sequential switch to move from one to another electrode and by the time necessary to read the potentiometri c signal. The analogue switch, the interface board and computer control software employed allowed a minimum switching time of 100 ms. It means that about 10 000 measurements of any individual electrode can be performed per second. For an array of eight electrodes, data can be acquired for each electrode at 1250 s¡1 . Note that the sampling rate provided by the circuitry and computer is fast enough when compared with the ¯ ow parameters and electrode responses, which, therefore, are the limiting factors of sample throughput. Results and discussion Evaluation of the potentiometer with the Ag‡ electrode array The potentiometer constructed was evaluated for its capability of random access to any electrode of the array of seven silver sulphide electrodes and to verify the performance of the summing circuit. In this case, solutions containing silver ions from 1:0 £ 10¡1 to 1:0 £ 10¡5 mol l¡1 were continuously pumped at 4.0 ml min¡1 through the electrode array. Usually the responses of the electrodes are slightly diå erent from each other, this behaviour being explained based on the process of manufacturing and maintenance of the solid membranes. Hence, of the seven electrodes, two presented a Nernstnian response (59.6 mV per decade of concentration), three showed a sub-Nernstnia n response and two a superNernstnian response (table 1). The response produced when more than one electrode was connected to the summing circuit showed that the individual responses are additive, independent of the Table 1. Results obtained in a continuous £ow system for the calibration of the silver-selective electrodes in the concentration ¡5 ¡1 ¡1 range from 1.0 £ 10 to 1.0 £ 10 mol l . Electrode 1 2 3 4 5 6 7 Slope (mV/pAg) 53.0 54.0 61.0 58.5 48.0 65.5 64.5 Linear coeæ cient (mV) 425 437 459 448 409 460 449 Correlation 0.9998 0.9991 0.9999 0.9999 0.9981 0.9951 0.9962 Table 2. Results obtained in the FIA and MSFA systems for the calibration of K + , Ca2 + and Cl- electrodes in ¡5 ¡1 ¡1 the concentration range from 1.0 £ 10 to 1.0 £ 10 mol L . FIA K‡ Slope (mV/pIon) Linear coeæ cient (mV) LOD (mol l71 ) Correlation 51 7125 ¡5 1:0 £ 10 0.9994 Ca2‡ 24 21 3:0 £ 10 ¡6 0.997 Cl¡ 754 7100 ¡5 3:1 £ 10 0.998 K‡ 52 7128 0.9996 MSFA Ca2‡Š23 18 0.993 Cl¡ 752 796 0.999 potential (mV) 200 100 0 Cl - (A) -100 -200 -300 0 300 potential (mV) 200 100 0 -100 -200 -300 -400 0 200 400 600 800 1000 1200 time (s) Ca2+ Cl K Ca 100 200 300 400 500 time (s) + 2+ The signals shown in ® gure 4 were obtained by the injection of 500 ml reference solutions containing the three ions. Typical signals, obtained by sequential reading of the electrodes, showed no signi® cant diå erence from those obtained by reading only one electrode each time for both the FIA and the MSFA systems. In the MSFA system, the air bubbles restrict the sample dispersion and the measurements resemble those of a conventional batch procedure, showing a staircase pro® le. The sequential measurements of the electrodes started when the sample monosegment reaches the reference electrode (detected by a regular potential reading for the last electrode in the array), ensuring that the array and reference electrode are in electrical contact through the monosegment solution. Table 2 shows the results obtained for K‡ , Ca2‡ and Cl¡ ions by employing the FIA and the MSFA systems. The MSFA approach presented no signi® cant advantage over the FIA system in the present case as the sensitivity (and even the washing time) was not improved. However, MSFA can present some advantage for sensors with lower response times as the ¯ ow can be easily stopped (by switching valve V in ® gure 2) when the sample monosegment is inside the system, and a long enough waiting time can be used to attain a suitable response. The MSFA approach can also facilitate standard addition procedures commonly employed to overcome matrix eå ects in potentiometry, as the same sample aliquot can be employed in this process [21]. The sample throughput for both ¯ ow systems was about 90 h¡1 . As three sensors were monitored after one sample introduction, the number of determinations were 270 h¡1 . A system with an array of eight electrodes for eight diå erent analytes will perform 720 determinations per hour, without any signal distortion, ensured by the higher sampling rate of the multichannel potentiometer. Preliminary evaluation of the potentiometer for Hadamard multiplexed reading The Hadamard approach for data acquisition requires the electrode readings to be combined in a pre-established way guided by a Simplex matrix [22± 24]. The individual signals can be recovered after a mathematical transformation (Hadamard Transform or demultiplexation). The signals thus obtained present a gain in the signal-to-nois e ratio known as multiplex gain, which is equal to the square root of two to a power determined by (B) K+ Figure 4. Pro¢le of the signal obtained for Cl¡ , Ca2‡ and K‡ electrodes in (A) FIA system and (B) MSFA system. It has been demonstrated that the washing time for the ¯ ow-through electrodes is decreased by employing higher carrier ¯ ow rates in the system, as the surface of the electrode is cleaned mainly due to diå usion eå ects, as a consequence of the laminar ¯ ow usually found in these systems [4]. Therefore, values around 8.0 ml min¡1 have been employed for both the FIA and the MSFA approaches. The multichannel potentiometer can deal with such a high ¯ ow rates without losing information coming from the electrodes of the array. In fact, both the FIA and the MSFA signals can be fully recovered at the sampling rate achieved by the instrument for all three indicator electrodes, as can be noted in ® gure 4. the number of electrodes minus one, divided by two. However, this gain is attained only if the noise remains constant and is limited by the sensor that produces the multiplexed signal [22]. Recently, it has been demonstrated that voltammetric signals obtained with the Hadamard approach from an array of ultra-microelectrodes show a gain in the signal-to-nois e ratio within the expected value predicted by the multiplex theory. The multiplex strategy has not been evaluated for the potentiometric electrochemical measurements made with arrays of electrodes. A preliminary evaluation of the potentiometer was carried out, considering its further application to perform Hadamard multiplexed reading of the electrodes in the array. The potentiometer constructed allows connecting the electrodes to produce the multiplexed reading of a Hadamard matrix of order 2n ¡ 1 (here n ˆ 2) [22]. The lines of the Hadamard multiplex matrix would be (1 1 0), (1 0 1) and (0 1 1). The digit (1) means that the electrode participates (is connected) in the total multiplexed signal measured, while (0) means that the electrode is not connected. Then, the three multiplexed signals obtained under computer control would be submitted to a Hadamard transform mathematical operation (demultiplex) [22], regenerating the individual responses for each sensor. Note that when using the Hadamard approach, three multiplexed reading measurements are made and each electrode is read twice. It has been demonstrated that this approach results in a better limit of detection for spectrophotometri c [25] and voltammetric [14] measurements. In addition, the multiplexed reading presents the Felgett gain, which can predicts that (N ¡ 1) measurements of the same sensor are performed in the same time interval of a single measurement of a sequential reading of an array of N sensors. This gain results in a better precision of the response produced for each sensor, considering the same interval of time for measurements. To mimic the Hadamard multiplexed measurements, three chloride electrodes were evaluated regarding the limit of detection and precision. Table 3 lists the results obtained with a single electrode and those obtained by summing the potential of these three electrodes. The limit of detection, determined according to the IUPAC recommendations for selective electrodes [26], does not show any improvement when the responses of the electrodes are summed up by the instrument. This behaviour was expected as the detection limits in potentiometri c sensors are de® ned by the chemical equilibrium associated to the species that participate in the membrane composition and with the response mechanism, instead of instrumental (electronic) parameters. However, the precision of the measurements for concentrations above the detection limit is improved due the increase in the potentiometri c signal when the response of more than one electrode are added. As the potential value has increased due to the sum, the relative standard deviation has been improved. Considering the behaviour of the signal precision as a function of the number of electrodes employed in a measurement, it is possible to predict the use of the multichannel potentiometer in more complex measurement protocols, as in the Hadamard multiplexed approach. This type of measurement would, at least, ensure an increase in the precision of individual readings Table 3. Limits of detection for Cl electrodes, considering individual measurements and the sum of their responses. Electrode 1 2 3 1+ 2+ 3 Blank signal (mV) 211 206 210 496 sd (mV) 2 3 2 2 LOD (mol L¡1 ) 3:1 £ 10¡5 2:3 £ 10¡5 2:4 £ 10¡5 1:7 £ 10¡5 ¡ of each electrode, without increasing the measurement time, as previously observed for voltammetric measurements [14]. Conclusions The multichannel potentiometer proposed here is a versatile, low-cost instrument that can improve potentiometric measurements. It allows one to access arrays of electrodes at a rate high enough for the most common ¯ ow analysis techniques such as FIA and MSFA. The number of determinations increases with the number of ion-selective electrodes in the array times the sampling frequency allowed by the ¯ ow system, reducing, as a consequence, sample consumption. In the present work, a sampling frequency of 270 h¡1 was achieved, as three selective electrodes were used in the array and 90 samples were processed per hour. Besides these advantages , the instrument permits the grouping of two or more selective electrodes for the same analyte, improving the signal magnitude for that species, as well as Hadamard multiplexed data acquisition. The adoption of this last approach would result in an additional gain in the precision of the potentiometric measurements. Acknowledgements Authors are grateful to ICCTI (Portugal) and CAPES (Brazil) for ® nancial support and to Professor C. H. Collins for the English revision of the manuscript. http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Journal of Automated Methods and Management in Chemistry Hindawi Publishing Corporation

Design and development of a multichannel potentiometer for monitoring an electrode array and its application in flow analysis

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Hindawi Publishing Corporation
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Copyright © 2002 Hindawi Publishing Corporation.
ISSN
1463-9246
eISSN
1464-5068
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Abstract

Instituto de Qu|mica, UNICAMP, CP 6154, CEP 13083-970, Campinas, è Brazil 2 CEQUP, Departamento de Qu|mica-F|èsica, Faculdade de Farmacia, Porto, è è Portugal A versatile potentiometer that works with electrode arrays in £ow injection and/or monosegmented £ow systems is described. The potentiometer is controlled by a microcomputer that allows individual, sequential multiplexed or random accesses to eight electrodes while employing only one reference electrode. The instrument was demonstrated by monitoring an array of seven £ow-through ion-selective electrodes for Ag‡ and for three electrodes for Cl¡ , Ca2‡ and K‡ . The ¢gures of merit of the individual and multiplexed (summed) readings of the electrode array were compared. The absolute standard deviation of the measurements made by summing the potential of two or more electrodes was maintained constant, thus improving the precision of the measurements. This result shows that an attempt to combine the signals of the electrodes to produce a more intense signal in the Hadamard strategy is feasible and accompanied by a proportional improvement in the precision of individual measurements. The preliminary tests suggest that the system can allow for 270 determinations per hour, with a linear range from 1:0 £ 10¡2 to 1:0 £ 10¡4 mol l¡1 for the three di¡erent analytes. Detection limits were estimated as 3 :1 £ 10¡5 , 3 :0 £ 10¡6 and 1:0 £ 10¡5 mol l¡1 for Cl¡ , Ca2‡ and K‡ , respectively. Introduction Potentiometric analytical methodologies have been widely employed for implementing online measurements owing to the ruggedness and selectivity of the sensors, which can be produced for many species of interest in the ® eld of agriculture [1], environmental chemistry [2] and clinical chemistry [3]. Ion-selective electrodes can be easily constructed, showing good analytical performance for the linear response range, selectivity, precision and lifetime. This kind of electrode is easy to miniaturize and can be arranged in arrays [4± 7]. The well-established ¯ ow techniques such as ¯ ow injection analysis (FIA) [8] and monosegmented ¯ ow analysis (MSFA) [9] can also be used for sample presentation and management (dilution and conditioning) in order to expand the useful concentration range and increase sample throughput. * To whom correspondence should be addressed. The goals of using an electrode array are to enhance the sensitivity and selectivity of the potentiometri c methodologies and/or to perform simultaneous determinations. Sensitivity can be improved by connecting the electrodes in series [10,11], which requires the use of several reference electrodes, even though a conventional monochannel potentiometer can be used. This approach is feasible only for determination of a single species, providing an increase in the slope of the analytical curve equivalent to the sum of the slopes of each electrode employed in the array. A simple alternative to double the sensitivity in ¯ ow injection potentiometry is achieved by placing two of the same ion-selective electrode in a single-line ¯ ow injection manifold where they work alternately as the reference electrode and the indicator electrode [4]. This approach provides an analytical signal similar to the pro® le of a second derivative of a potentiometric titration curve and the distance between the two electrodes should be optimized to obtain maximum sensitivity. The sensitivity of potentiometric measurements can also be improved by employing multichannel instruments [4,12]. The simplest version of this kind of potentiometer allows the electronic summing of the potential of a few electrodes (two or three) and employs only one reference electrode [4]. The capabilities of such potentiometers can be further expanded to allow simultaneous determinations if the electrodes of an array can be individually accessed. Furthermore, the instrument should be versatile to allow for summing up of the responses of more than one electrode and to perform any kind of readout from an individual reading to multiplexed readings, such as those necessary for the Hadamard multiplex approach [13± 15]. Most commercial potentiometers are monochannel instruments and access to the individual sensors of an electrode array cannot be made easily. Although recently some instrument manufacturers have oå ered multichannel instruments, the associated software is not suæ ciently ¯ exible to allow full user-tailored data acquisition [16]. Some contributions have been described in the literature for the development of multichannel potentiometers. Couto et al. [4] described a three-channel summing circuit for increasing the sensitivity of the potentiometric measurements, although the electrodes cannot be individually accessed. Alexander et al. [12] developed a multichannel circuit that can monitor up to six analytes simultaneously, but which employs a reference electrode for each indicator electrode. Forster and Diamond [6] used a four-channel potentiometer to perform non-linear calibration of ion-selective electrode arrays, where one of the electrodes should contain the ionophores of the three ISE. Although these contributions can either improve the sensitivity of the measurements [12] or perform simulta105 Journal of Automated Methods & Management in Chemistry ISSN 1463± 9246 print/ISSN 1464± 5068 online # 2002 Taylor & Francis Ltd http://www.tandf.co.uk/journals neous determinations [6], they do not provide random access to the electrodes or multiplexing reading, which is necessary for the Hadamard multiplexed approach. This paper describes a multichannel potentiometri c instrument, which is versatile to permit data acquisition in any user-selected form. The instrument has been evaluated for its ability to sum up the potential produced by many electrodes selective to the same analyte (Ag ‡ ) and to access the individual reading of an array containing three selective electrodes for Cl¡ , Ca2‡ and K ‡ . An evaluation of the instrument was made for operation with FIA and MSFA manifolds and for individual (sequential/random) or Hadamard multiplexed measurements. LM 348 + + + + + + + + ADG 201A To computer IE1 IE2 IE3 0.1 mF IE4 To A/D CA 3140 IE5 RE IE6 IE7 Materials and methods Reagents All reagents were of analytical grade and the solutions were prepared by using distilled and deionized water. The Ag‡ solutions in the 1:0 £ 10¡1 to 1:0 £ 10¡4 mol l¡1 concentration range were prepared by diluting a 1.0 mol l¡1 AgNO 3 stock solution. Solutions containing K‡ , Ca2‡ and Cl¡ ions in the 1:0 £ 10¡1 to 1:0 £ 10¡5 mol l¡1 concentration range were also prepared by proper dilution of 1.0 mol l¡1 KNO3 , Ca(NO3 )2 and NaCl stock solutions. The ionic strength of all solutions was adjusted to 1.0 mol l¡1 with a NaNO 3 solution. Multichannel potentiometer Figure 1 shows the electronic layout of the multichannel potentiometer constructed. The electronic circuit of the instrument is very simple and has been conceived to operate with up to eight selective electrodes and only one reference electrode. Each indicator electrode is connected to a high-impedance FET operational ampli® er (LM348) mounted in a buå er con® guration. The selection of the electrode (or electrodes) that will produce the signal is made through two four-input analogue switches (ADG 201A). The control of the switches is made by a computer interface (PCL-711S, Advantech), through eight digital outputs. The signal (or the sum of the signals if more than one electrode is simultaneousl y connected) is sent to the inverter input of a high-impedance operational ampli® er (CA3140). The reference electrode is connected to the non-inverter input of this operational ampli® er. When only one electrode is connected, the circuit works as a comparator. The same circuit acts as a summing point, adding the electrochemical potential diå erences generated by more than one electrode when they are simultaneously selected to participate in the measurement of a single species. Flow system Figure 2 shows a schematic diagram of the ¯ ow system employed. The system employs a four-channel peristaltic pump (Ismatec MS-Reglo) and a proportional injector IE8 Figure 1. Electronic circuit of the multichannel potentiometer. To computer OS RE C V Air A L L ISEA S I Figure 2. Schematic diagram of the £ow manifold. C, carrier £uid; P, peristaltic pump; V, three-way solenoid valve; L1/L2, air loops; A, sample loop; S, sample; OS, optical switch; ISEA, ion-selective electrode array; RE, reference electrode; W, waste. [17] to insert the sample into a MSFA or into a FIA (without the air loops, L1 and L2 ) manifold. An optoswitch (OS) is coupled to the sliding bar of the injector in order to ¯ ag each sample injection for the computer. The manifold includes a three-way solenoid valve (NResearch), placed before the proportional injector and used to deviate the carrier ¯ ow for stopped ¯ ow measurements. The electrode array was placed 10 cm from the injection port. The reference electrode was a standard double junction calomel (Corning Ð 900200), ® lled with a 1.0 mol l¡1 NaNO 3 external solution and placed after (at 1.0 cm) the electrode array. Tygon pumping tubes and polyethylene conducting tubes (0.8 mm i.d.) were employed throughout . The carrier solution was always a 1.0 mol l¡1 NaNO 3 solution. Electrode arrays Two electrode arrays were employed in the present study. The ® rst was used to investigate the performance of the potentiometer regarding its capability of adding the electrochemical potentials generated by each indicator electrode. The array contained seven silver sulphide ¯ ow-through electrodes with internal diameters of Potential (mV) 1.0 mm [18]. These 1.0 mm-thick electrode discs were arranged in series inside acrylic rods having a 15 mm external diameter and spaced from each other by 4.0 mm. The other array was built with three diå erent membrane-selective electrodes for K‡ , Ca2‡ and Cl¡ . The metal ion-selective electrodes were based on polymeric liquid membranes, constructed as described [19, 20], while the chloride-selective electrode was constituted by an AgCl/Ag2 S solid membrane [18]. This array was employed to evaluate the multiplexing and sequential reading capabilities of the potentiometer. Computer and software resources The multichannel potentiometer was controlled by an IBM-compatible 300 MHz PC-486 furnished with a PCL-711S (Advantech) parallel interface. This interface has a 12-bit analogue-to-digita l converter with a conversion rate of 100 kHz. Eight digital outputs of the interface were employed for electrode selection. Software written in Microsoft VisualBasic 5.0 was developed for electrode selection and acquisition, treatment and the storage of data. linear = - 2,57 slope = 400,6 r = 0,99994 3 4 5 6 7 number of electrodes Figure 3. Potential observed as a function of the number of silver electrodes used in the measurement for a 1:0 £ 10¡1 mol l¡1 Ag‡ solution. number and of which electrodes were selected to comprise the ® nal potentiometric signal. Figure 3 shows the signal as a function of the number of the electrodes that participate in the measurement; the straight line obtained presents a slope of 400.5 mV, very close to the sum (404.5 mV) of the individual slopes listed in table 1. This result also demonstrates that the electronic circuit of the multichannel potentiometer does not distort the signal when the electrical potentials of the indicator electrodes are summed, in accordance to the results obtained by Couto et al. [4] for summing two electrodes. In addition, the linearity of the response as a function of the concentration of Ag‡ ions is maintained from 10¡4 up to 10¡1 mol l¡1 , with a regression coeæ cient of 0.9996. Evaluation of the potentiometer with the K‡ , Ca2‡ and Cl¡ electrode array This array was evaluated for use with FIA and MSFA systems. In this case, the sampling rate of the signals produced by the diå erent indicator electrodes must be high enough to allow the sequential monitoring of the sensors. The sampling rate was determined by the time necessary for the sequential switch to move from one to another electrode and by the time necessary to read the potentiometri c signal. The analogue switch, the interface board and computer control software employed allowed a minimum switching time of 100 ms. It means that about 10 000 measurements of any individual electrode can be performed per second. For an array of eight electrodes, data can be acquired for each electrode at 1250 s¡1 . Note that the sampling rate provided by the circuitry and computer is fast enough when compared with the ¯ ow parameters and electrode responses, which, therefore, are the limiting factors of sample throughput. Results and discussion Evaluation of the potentiometer with the Ag‡ electrode array The potentiometer constructed was evaluated for its capability of random access to any electrode of the array of seven silver sulphide electrodes and to verify the performance of the summing circuit. In this case, solutions containing silver ions from 1:0 £ 10¡1 to 1:0 £ 10¡5 mol l¡1 were continuously pumped at 4.0 ml min¡1 through the electrode array. Usually the responses of the electrodes are slightly diå erent from each other, this behaviour being explained based on the process of manufacturing and maintenance of the solid membranes. Hence, of the seven electrodes, two presented a Nernstnian response (59.6 mV per decade of concentration), three showed a sub-Nernstnia n response and two a superNernstnian response (table 1). The response produced when more than one electrode was connected to the summing circuit showed that the individual responses are additive, independent of the Table 1. Results obtained in a continuous £ow system for the calibration of the silver-selective electrodes in the concentration ¡5 ¡1 ¡1 range from 1.0 £ 10 to 1.0 £ 10 mol l . Electrode 1 2 3 4 5 6 7 Slope (mV/pAg) 53.0 54.0 61.0 58.5 48.0 65.5 64.5 Linear coeæ cient (mV) 425 437 459 448 409 460 449 Correlation 0.9998 0.9991 0.9999 0.9999 0.9981 0.9951 0.9962 Table 2. Results obtained in the FIA and MSFA systems for the calibration of K + , Ca2 + and Cl- electrodes in ¡5 ¡1 ¡1 the concentration range from 1.0 £ 10 to 1.0 £ 10 mol L . FIA K‡ Slope (mV/pIon) Linear coeæ cient (mV) LOD (mol l71 ) Correlation 51 7125 ¡5 1:0 £ 10 0.9994 Ca2‡ 24 21 3:0 £ 10 ¡6 0.997 Cl¡ 754 7100 ¡5 3:1 £ 10 0.998 K‡ 52 7128 0.9996 MSFA Ca2‡Š23 18 0.993 Cl¡ 752 796 0.999 potential (mV) 200 100 0 Cl - (A) -100 -200 -300 0 300 potential (mV) 200 100 0 -100 -200 -300 -400 0 200 400 600 800 1000 1200 time (s) Ca2+ Cl K Ca 100 200 300 400 500 time (s) + 2+ The signals shown in ® gure 4 were obtained by the injection of 500 ml reference solutions containing the three ions. Typical signals, obtained by sequential reading of the electrodes, showed no signi® cant diå erence from those obtained by reading only one electrode each time for both the FIA and the MSFA systems. In the MSFA system, the air bubbles restrict the sample dispersion and the measurements resemble those of a conventional batch procedure, showing a staircase pro® le. The sequential measurements of the electrodes started when the sample monosegment reaches the reference electrode (detected by a regular potential reading for the last electrode in the array), ensuring that the array and reference electrode are in electrical contact through the monosegment solution. Table 2 shows the results obtained for K‡ , Ca2‡ and Cl¡ ions by employing the FIA and the MSFA systems. The MSFA approach presented no signi® cant advantage over the FIA system in the present case as the sensitivity (and even the washing time) was not improved. However, MSFA can present some advantage for sensors with lower response times as the ¯ ow can be easily stopped (by switching valve V in ® gure 2) when the sample monosegment is inside the system, and a long enough waiting time can be used to attain a suitable response. The MSFA approach can also facilitate standard addition procedures commonly employed to overcome matrix eå ects in potentiometry, as the same sample aliquot can be employed in this process [21]. The sample throughput for both ¯ ow systems was about 90 h¡1 . As three sensors were monitored after one sample introduction, the number of determinations were 270 h¡1 . A system with an array of eight electrodes for eight diå erent analytes will perform 720 determinations per hour, without any signal distortion, ensured by the higher sampling rate of the multichannel potentiometer. Preliminary evaluation of the potentiometer for Hadamard multiplexed reading The Hadamard approach for data acquisition requires the electrode readings to be combined in a pre-established way guided by a Simplex matrix [22± 24]. The individual signals can be recovered after a mathematical transformation (Hadamard Transform or demultiplexation). The signals thus obtained present a gain in the signal-to-nois e ratio known as multiplex gain, which is equal to the square root of two to a power determined by (B) K+ Figure 4. Pro¢le of the signal obtained for Cl¡ , Ca2‡ and K‡ electrodes in (A) FIA system and (B) MSFA system. It has been demonstrated that the washing time for the ¯ ow-through electrodes is decreased by employing higher carrier ¯ ow rates in the system, as the surface of the electrode is cleaned mainly due to diå usion eå ects, as a consequence of the laminar ¯ ow usually found in these systems [4]. Therefore, values around 8.0 ml min¡1 have been employed for both the FIA and the MSFA approaches. The multichannel potentiometer can deal with such a high ¯ ow rates without losing information coming from the electrodes of the array. In fact, both the FIA and the MSFA signals can be fully recovered at the sampling rate achieved by the instrument for all three indicator electrodes, as can be noted in ® gure 4. the number of electrodes minus one, divided by two. However, this gain is attained only if the noise remains constant and is limited by the sensor that produces the multiplexed signal [22]. Recently, it has been demonstrated that voltammetric signals obtained with the Hadamard approach from an array of ultra-microelectrodes show a gain in the signal-to-nois e ratio within the expected value predicted by the multiplex theory. The multiplex strategy has not been evaluated for the potentiometric electrochemical measurements made with arrays of electrodes. A preliminary evaluation of the potentiometer was carried out, considering its further application to perform Hadamard multiplexed reading of the electrodes in the array. The potentiometer constructed allows connecting the electrodes to produce the multiplexed reading of a Hadamard matrix of order 2n ¡ 1 (here n ˆ 2) [22]. The lines of the Hadamard multiplex matrix would be (1 1 0), (1 0 1) and (0 1 1). The digit (1) means that the electrode participates (is connected) in the total multiplexed signal measured, while (0) means that the electrode is not connected. Then, the three multiplexed signals obtained under computer control would be submitted to a Hadamard transform mathematical operation (demultiplex) [22], regenerating the individual responses for each sensor. Note that when using the Hadamard approach, three multiplexed reading measurements are made and each electrode is read twice. It has been demonstrated that this approach results in a better limit of detection for spectrophotometri c [25] and voltammetric [14] measurements. In addition, the multiplexed reading presents the Felgett gain, which can predicts that (N ¡ 1) measurements of the same sensor are performed in the same time interval of a single measurement of a sequential reading of an array of N sensors. This gain results in a better precision of the response produced for each sensor, considering the same interval of time for measurements. To mimic the Hadamard multiplexed measurements, three chloride electrodes were evaluated regarding the limit of detection and precision. Table 3 lists the results obtained with a single electrode and those obtained by summing the potential of these three electrodes. The limit of detection, determined according to the IUPAC recommendations for selective electrodes [26], does not show any improvement when the responses of the electrodes are summed up by the instrument. This behaviour was expected as the detection limits in potentiometri c sensors are de® ned by the chemical equilibrium associated to the species that participate in the membrane composition and with the response mechanism, instead of instrumental (electronic) parameters. However, the precision of the measurements for concentrations above the detection limit is improved due the increase in the potentiometri c signal when the response of more than one electrode are added. As the potential value has increased due to the sum, the relative standard deviation has been improved. Considering the behaviour of the signal precision as a function of the number of electrodes employed in a measurement, it is possible to predict the use of the multichannel potentiometer in more complex measurement protocols, as in the Hadamard multiplexed approach. This type of measurement would, at least, ensure an increase in the precision of individual readings Table 3. Limits of detection for Cl electrodes, considering individual measurements and the sum of their responses. Electrode 1 2 3 1+ 2+ 3 Blank signal (mV) 211 206 210 496 sd (mV) 2 3 2 2 LOD (mol L¡1 ) 3:1 £ 10¡5 2:3 £ 10¡5 2:4 £ 10¡5 1:7 £ 10¡5 ¡ of each electrode, without increasing the measurement time, as previously observed for voltammetric measurements [14]. Conclusions The multichannel potentiometer proposed here is a versatile, low-cost instrument that can improve potentiometric measurements. It allows one to access arrays of electrodes at a rate high enough for the most common ¯ ow analysis techniques such as FIA and MSFA. The number of determinations increases with the number of ion-selective electrodes in the array times the sampling frequency allowed by the ¯ ow system, reducing, as a consequence, sample consumption. In the present work, a sampling frequency of 270 h¡1 was achieved, as three selective electrodes were used in the array and 90 samples were processed per hour. Besides these advantages , the instrument permits the grouping of two or more selective electrodes for the same analyte, improving the signal magnitude for that species, as well as Hadamard multiplexed data acquisition. The adoption of this last approach would result in an additional gain in the precision of the potentiometric measurements. Acknowledgements Authors are grateful to ICCTI (Portugal) and CAPES (Brazil) for ® nancial support and to Professor C. H. Collins for the English revision of the manuscript.

Journal

Journal of Automated Methods and Management in Chemistry – Hindawi Publishing Corporation

Published: Sep 14, 2014

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