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A Full Automatic Device for Sampling Small Solution Volumes in Photometric Titration Procedure Based on Multicommuted Flow System

A Full Automatic Device for Sampling Small Solution Volumes in Photometric Titration Procedure... 1 Centro 2 Centro de Energia Nuclear na Agricultura, Universidade de S˜ o Paulo, Avenida Centen´ rio 303, 13400-970 Piracicaba, SP, Brazil a a de Ciˆncias Exatas e Tecnol´gicas, Universidade Federal do Recˆncavo da Bahia, 44380-000 Cruz das Almas, BA, Brazil e o o Received 9 April 2007; Accepted 7 June 2007 In this work, an automatic device to deliver titrant solution into a titration chamber with the ability to determine the dispensed volume of solution, with good precision independent of both elapsed time and flow rate, is proposed. A glass tube maintained at the vertical position was employed as a container for the titrant solution. Electronic devices were coupled to the glass tube in order to control its filling with titrant solution, as well as the stepwise solution delivering into the titration chamber. The detection of the titration end point was performed employing a photometer designed using a green LED (λ = 545 nm) and a phototransistor. The titration flow system comprised three-way solenoid valves, which were assembled to allow that the steps comprising the solution container loading and the titration run were carried out automatically. The device for the solution volume determination was designed employing an infrared LED (λ = 930 nm) and a photodiode. When solution volume delivered from proposed device was within the range of 5 to 105 μl, a linear relationship (R = 0.999) between the delivered volumes and the generated potential difference was achieved. The usefulness of the proposed device was proved performing photometric titration of hydrochloric acid solution with a standardized sodium hydroxide solution and using phenolphthalein as an external indicator. The achieved results presented relative standard deviation of 1.5%. Copyright © 2007 Sivanildo S. Borges et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. INTRODUCTION Generally, in automatic titration procedure based on flow injection analysis process, the volume of the titrant solution delivered has been determined considering both flow rate and time interval elapsed while the titration was run [1–3]. In principle, it has been admitted that the flow rate was constant and the time interval was a very well-controllable variable [4, 5]. In these cases, peristaltic pump has been the device widely used to propel titrant solution [6–8]. Because pumping pulsation, due to peristaltic pump, could impair the precision of the delivered solution volume, a synchronization strategy has been implemented [4, 9]. Since peristaltic pump maintain a constant pulsation pattern, small volume of titrant solution, presenting good precision, could be delivered. Nevertheless, to accomplish this requirement, it is necessary to resort facilities comprising electronic and software [4, 9, 10]. Furthermore, the aging of the pumping tube could affect flow rate, thus this effect could become an error source. In this work, we intend to develop a device with ability to deliver small aliquots of titrant solution, determining also its volume with good precision and accuracy independent of both time and flow rate. The usefulness of the device will be demonstrated, coupling then to an automatic titration module based on multicommutation process [11, 12]. 2. 2.1. EXPERIMENTAL Solutions Purified water with electric conductivity less than 0.1 μS cm−1 was used throughout. An 89.2 ± 0.9 molL−1 HCl solution was prepared by dilution from a 1 molL−1 HCl solution. This solution was standardized by titration using an 88.7±0.8 molL−1 NaOH solution, which was previously standardized by titration using a potassium biphthalate solution and a 0.01% (w/v) phenolphthalein solution as indicator. 2.2. Apparatus The equipment set up comprised a Pentium III microcomputer furnished with an electronic interface card (PCL-711S, Advantech), an IPC-4 Ismatec peristaltic pump with Tygon PD Col Opt HC TR Pht LED BS B 30 cm TC CD LED1 (a) V1 TC AP (b) Tch V2 (c) Figure 1: View of the volume meter. (a) Detailed description of the device: TC = solution container, glass tube 30 cm long, 0.5 cm and 0.35 cm external and inner diameters, respectively; CD = solution inlet/outlet; B = floating device, polyethylene vial (transparent) with flat bottom, 25 mm long, 3.4 mm external diameter, 0.5 mm wall thickness; LED and LED1 = infrared light emitting diode (λ = 930 nm); Pht = phototransistor (Til78); Col = light beam collimator, metallic piece with dimension of 9 cm2 surface, 3.5 cm thickness, and central hole (1.0 mm diameter) for light transmission; PD = photodiode (Hamamatsu, S1337-1010BR). (b) Solution container hold; AP = acrylic plate with dimension of 15 × 20 × 1.5 cm; BS = brass cylinder, 30 cm long and 1.0 cm diameter; HC = glass tube holder, acrylic plate with dimension 15 × 10 × 1 cm. (c) Assembling view of the volume meter: TR = reservoir of titrant solution; V1 = pinch solenoid valve normally closed; V2 = three-way solenoid valve; Tch = titration chamber (14). Solid and doted lines into the valve (V2 ) symbol indicate the fluid pathway when valve was switched OFF and ON, respectively. pumping tubes, six three-way solenoid valves (161T031, Nresearch), one solenoid pinch valve normally closed (161P011, Nresearch), a homemade 12 V regulated power supply to feed the solenoid valves, a homemade electronic interface [13] to provide the potential difference and current intensity required to drive the solenoid valves, and a homemade photometric detector [14]. The control unit comprised one photodiode (Hamamatsu, S1337-1010BR), one phototransistor (Til78) wired as an optic switch, two infrared LED (λ = 930 nm), two operational amplifiers (OP07), one comparator device (LM339), and one transistor (BC547). The assays comprising the volume meter calibration and photometric titration were performed employing a software wrote in Quick BASIC 4.5. Flow lines were of Tygon tubing 0.56 mm inner diameter. 2.3. The volume meter description In Figure 1, it is shown a front view of the volume meter, where we can see that the device is coupled to the titrant solution reservoir (TR) through the solenoid valves V1 and V2 . The V2 was assembled to permit the container loading (TC) with titrant solution when valve V1 was switched ON. When the container was filled with titrant solution, the floating device (B) interrupted the infrared radiation beam of the optic switch (Opt). When the electronic interface showed in Figure 2 sensed the interruption of the radiation beam, it generated the control signal to switch OFF valve V2 in order to stop the stream of the titrant solution. 12 V 1k LED B 10 k 4 Opt 5V Pht1 5 + −1 4 LM339 10 k D0 Pw V1 12 V TC 20 k 12 V Ens Figure 2: Diagram of the device to control the filling of the titrant solution container. Opt = optic switcher, LED = infrared emitting diode (930 nm), Pht = phototransistor (Til78), Pw = power driving device (ULN2803), D0 = Pw first input line, V1 = pinch solenoid valve normally closed, Ens = control enabling line. The optic switch (Opt) comprising an infrared radiation emitting diode (λ = 930 nm) and a phototransistor (Til78), which was attached in a metallic piece (5 × 5 × 0.4 cm) with a central lead hole to permit the inserting of the solution container (TC), thus allowing that the container was positioned between the phototransistor (Pht) and the infrared LED. A hole with a diameter of 1.0 mm was drilled at the orthogonal position to the lead hole in order to permit that the infrared Sivanildo S. Borges et al. Table 1: Steps sequence of the titration procedure. Step 0 1 2 3 4 5 6 7 8 9 10 11 ∗ V1 0 1 0 0 0 0 0 0 0 0 0 0 V2 0 0 0 0 0 0 0 0 0 0 1 0 V3 0 0 0 0 0 1 0 0 0 1 0 0 ∗∗ V4 0 0 0 0 0 1 0 0 0 1 0 0 V5 0 0 0 1 0 0 0 1 0 0 0 0 V6 0 0 0 1 0 0 0 0 1 0 0 0 ∗∗∗ V7 0 0 0 0 1 0 1 0 0 0 0 0 D0 Pw 0 1 0 0 0 0 0 0 0 0 0 0 Time (s) — — — 20 15 20 20 sit∗∗∗ 2 8 — — Description Standby Fill titrant container Standby Fill flow line S and In∗ Empting titration chamber Washing titration chamber∗∗ Empting titration chamber∗∗ Sample inserting time Indicator insertion Carrier solution insertion Start titration End titration S = sample, In = indicator solution; steps that were repeated twice; sit = value defined when the software was run. beam attained the phototransistor (Pht) after it crosses the titrant solution container (TC). As it is depicted in Figure 1, an infrared radiation emitting diode (LED1) was installed at the bottom of the titrant solution container (TC), thus the radiation beam emitted by this LED was directed towards the photodiode (PD) through the liquid column maintained inside of the container. The liquid column behaves as a wave guide and it was observed that its length affected the intensity of the infrared radiation beam that reaches the photodiode (PD). The volume meter was developed exploiting this effect. 2.4. The volume meter calibration The filling of titrant solution container (TC) was controlled by mean of the electronic interface showed in Figure 2. Prior to load the container with titration solution, the system was adjusted following the steps summarized in Table 1. Maintaining the titrant solution container empty, the signal generated by the optic switch (Opt) was 3.8 V that was applied to the no inverting input of the comparator device (LM339, pin 5). Reference signal applied to the comparator input (pin 4) was adjusted to 3.5 V turning the variable resistor (20 kΩ) wired to it. Under this condition, the output of the comparator device (pin 2) was at a high-state condition and the power-driving device (Pw) was maintained deactivate, while the control enabling line (Ens) was at low level (0 V). When the software was run, the microcomputer sent a control signal (TTL high level) through PCL711 interface card to enable the control line (Ens, Figure 2). Under this condition, the input line (D0 ) of the power-driving device (Pw) was enabled to switch ON valve V1 , thus the titrant solution flowed from its vessel (TR, Figure 1) by the gravity acceleration action to fill the titrant container (TC) with titrant solution. While the liquid column increased into the container, the floating device (B) was displaced toward the top. When it crossed the light beam of the optic switch (Opt), the signal sent to the comparator input (pin 5) fall lower than 3.0 V. Under this condition, the output signal of the comparator device (pin 2) was drove to the low-state condi- tion (0 V), thus disabling the line input (D0 ) of the powerdriving device (Pw), which switched OFF valve V1 in order to stop the stream of titrant solution. The light emitting diode (LED1) installed in the container bottom (TC, Figure 1) was switched OFF by turning the variable resistor wired to the base of the transistor (Tr1, Figure 3). The signal output (So) of the operational amplifier (OA2) was adjusted to 0 V by turning the variable resistor (20 kΩ) wired to the no inverting input of this operational amplifier. Afterwards, the emission intensity of the LED1 was raised up to the output signal (So) attained 2000 mV. This was done turning the variable resistor coupled to the base of the transistor (Tr1). The flow diagram of the titration system is shown in Figure 4. In this configuration, all valves are switched OFF, thus all solutions propelled by the peristaltic pump (PP) are directed towards their storing vessels. When valve V2 was switched ON, the titrant solution flowed through it. Aiming to find the relationship between the solution volumes delivered from the container (TC) and the output signal (So) generated by photodiode (Figure 3), a set of assays was carried out. The microcomputer sent, through the output port of the PCL711S interface card, a control signal to switch ON valve V2 . While solution flowed from the container (TC), the microcomputer read the variation of the signal (So) through the analog input of the PCL711S interface card. When signal variation attained a preset value (Vs), valve V2 was switched OFF in order to stop the solution stream, and the delivered volume of solution was measured. Assays were performed programming potentials difference ranging from 50 up to 800 mV. After calibration stage, the valve V2 was maintained switched ON during a time interval of 2 minutes to empty the titrant solution container. After calibration, a set of titration assays was carried out to demonstrate the usefulness of the proposed volume meter, which was implemented using the flow system showed in Figure 4, which was designed based on multicommutation process [10–12]. Titration chamber (Tch) and photometer detector (not showed) were similar to those employed in previous work [14]. 0.47 μF 10 M 12 V 5k 20 k 270 Tr1 LED1 PD 12 V 2 − 0.47 μF 470 k C1 12 V 100 k 2 C3 10 k S0 OA1 + 3 4 C2 −12 V − 7 6 OA2 + 3 4 C4 −12 V 100 k 20 k +12 V −12 V Figure 3: Electronic diagram of the interface to monitor the titrant solution into the container. Tr1 = transistor (BC547), LED1 = light emitting diode (930 nm), PD = photodiode (Hamamatsu, S1337-1010BR), OA1 e OA2 = operational amplifiers (OP07), C1, C2, C3, and C4 = 1 μF tantalum capacitors, So = signal output. Ri Rc PP In V3 V4 Cs V5 Rs S V7 V6 VM T Tch V2 PC TR V1 Table 2: Signal generated as function of the delivered water volume. Signal (mV) 56 100 140 165 234 273 318 372 463 559 791 Volume (μL) 5.7 10.3 14.9 19.0 28.0 32.6 38.4 46.4 58.7 72.5 103.9 Table 3: Comparison between the solution volumes measured and the preset values, results are average of three measurements. Figure 4: Diagram of the flow system. V1 , = pinch solenoid valve, V2 , V3 , V4 , V5 , V6 , and V7 = three way solenoid valves, S = sample; Cs = carrier solution, water, In = indicator, 0.01% (w/v) phenolphthalein solution, Rs, Rc, and Ri = solutions (S, Cs, In) circulation towards their storing vessels, respectively; W = waste, PP = peristaltic pump, T = titrant solution, 88.7 ± 0.8 molL−1 NaOH, Tch = titration chamber, TR = titrant solution reservoir, VM = volume meter (Figure 1), PC = microcomputer. Measured volume (μL)∗ 17.93 ± 0.06 29.40 ± 0.05 58.6 ± 0.7 76.7 ± 0.3 100.5 ± 0.6 ∗ Preset volume (μL) 17.7 ± 0.2 29.3 ± 0.3 58.8 ± 0.5 77.7 ± 0.4 99.6 ± 0.7 Values obtained weighting the delivered volume of water and considering the water density at 25◦ C. As it is depicted in Table 1, in the standby condition all valves are switched OFF, thus all solutions are pumped back to their storing vessels (Figure 4). When the software was started to carry out a titration run, the microcomputer sent a control signal (TTL high level) through the enabling line (Ens, Figure 2) to enable the power-driving device (Pw, Figure 2). Under this condition, valve V1 was switched ON to fill the container (TC) with titrant solution. This step was done as it was described in previous section. Afterwards, valves V5 and V6 were switched ON during a time interval of 20 seconds (step 3) to fill the flow lines up to the titration chamber (Tch). Afterwards, valve V7 was switched ON during a time interval of 15 seconds (step 4) to empty the titration chamber. The washing of the titration chamber with carrier solution comprised the steps 5 and 6 (Table 1), which were repeated twice to assure good cleaning. Following the working sequence showed in Table 1 (steps 7, 8), valves V5 and V6 were sequentially switched ON during preset time intervals to insert into the titration chamber aliquots of sample solution (S) and of indicator solution (In), Sivanildo S. Borges et al. Table 4: Comparison of the titration results, results are average of three consecutive titration run that were performed using a 88.7 ± 0.8 molL−1 NaOH standardized solution. Sample (HCl) 1 2 3 4 5 6 Sample volume (μL) 43 57 71 85 100 115 Actual HCl concentration (molL−1 ) 89.2 ± 0.9 89.2 ± 0.9 89.2 ± 0.9 89.2 ± 0.9 89.2 ± 0.9 89.2 ± 0.9 Found HCl concentration (molL−1 ) 89.5 ± 0.6 88.5 ± 0.9 89.1 ± 1.5 89.8 ± 0.5 88 ± 1 88 ± 1 Difference (%) −0.3 0.8 0.1 −0.7 1.3 1.3 respectively. The time interval to maintain valve V6 switched ON was settled at 2.0 seconds, while time for valve V5 was varied from 3.0 up to 8.0 seconds. Afterwards, valves V3 and V4 were switched ON during a time interval of 8.0 to insert 800 μl of the carrier solution into the titration chamber. As it is shown in Table 1 (step 10), valve V2 was switched ON to permit that the titrant solution flowed continuously by the gravity acceleration action toward the titration chamber (Tch). The monitoring of the signal generated by the photometer was performed by the microcomputer through the analog input of the PCL711S interface card. When a quick transition of the generated signal occurred, the microcomputer sent a control signal through the enabling line (Ens, Figure 2) to switch OFF valve V2 in order to stop the stream of the titration solution. This signal changing indicated that the stoichiometric condition was attained [14]. Afterwards, the microcomputer read the signal (S0 ) generated by the photodiode (PD) of the volume meter (Figure 3) that was saved as an ASCII file. The volume of the titrant solution used to find the end of titration was calculated using this measurement. When the signal (S0 ) surpassed a preset threshold value, which was related to a delivered solution volume of the titrant solution about 85 μl, the microcomputer halted the stream of the titrant solution and saved the signal value related with the solution volume that was used at that moment. Afterwards, the volume meter-filling step was carried out again and after that the titration run was reestablished in order to find the end of titration. 3. RESULTS AND DISCUSSIONS Volume meter calibration Intending to find the relationship between the volume of the solution delivered and the potential difference generated by the photodiode (PD), a set of assays was carried out yielding the results showed in Table 2. Processing these data, we found the following linear relationship: ΔE(mV) = −25.7 − 7.4 v(μL), (R = 0.999). Aiming to confirm the linear relationship, experiments were carried out at several days. The assays were done settling different values of potential difference and no significant difference was observed. Every day prior to begin the first titration run, the calibration stage was accomplished in order to find the parameters related to the linear relationship, which were incorporated in the control software to permit that the volume of titrant solution was calculated when titration run was ended. Intending to prove the ability of the device to deliver a preset solution volume, a set of experiments was performed using distilled water and results are showed in Table 3. Processing these data, a linear relationship presenting a slope of 0.999 and an intercept tending to 0.0 was achieved. These results indicated that the system was able to determine the solution volume processing the potential difference related to liquid column height. Furthermore, the precision of the delivered volumes was better than 1.0% (n = 10) which was confirmed repeating the experiments maintaining the preset values. 3.3. Automatic titration 3.1. General comments The volume meter working principle was based on the attenuation of the radiation beam intensity, which was affected by the height of the liquid column inserted between the electromagnetic radiation source (LED1, Figure 1) and the photodiode (PD). The value of the potential difference generated by the photodiode decreased when the gap between the liquid column top and the photodiode (PD) increased. Previous assays performed using LEDs with wavelength of 470 nm (blue), 650 nm (red), and 930 nm (infrared) showed that better linear range could be obtained with the infrared LED. In this sense, the results commented below were obtained employing this component. Aiming to demonstrate the usefulness of the proposed volume meter device, photometric titration of hydrochloric acid with sodium hydroxide solution was performed yielding the results showed in Table 4. The volumes of the HCl solution aliquots were varied from 43 up to 115 μL. As we can see the concentration of the HCl solution found is closed to expected values. In the assays labeled as 5 and 6 the volumes of the HCl solution aliquots used were 100 and 115 μL, respectively, thus the solution container (TC, Figure 1) was filled twice. Analyzing the results, we can see, that in both cases accuracy and precision were similar to the other ones showed in Table 4. 4. CONCLUSIONS The performance of the proposed volume meter shows that it can be used to deliver small volume with good precision 6 independent of the flow rate and the time interval. The instrumental arrangement is very simple and easy to be replicated in laboratory with a few little electronic facilities. The volume meter was successfully applied in the determination of the titrant solution volume in photometric titration procedure of hydrochloric acid with sodium hydroxide solution. Albeit, the operational work range was between 5 and 105 μL, the appropriated combination of software and hardware were able to refill the titrant solution container while the titration run was in course. The volume meter device presented a very good longterm stability, which was ascertained by working several days and no significant variation concerning to linear response range, precision, and accuracy was observed. ACKNOWLEDGMENTS ` Authors gratefully acknowledge the Fundacao de Amparo a ¸˜ Pesquisa do Estado de S˜o Paulo (FAPESP) and the Cona ´ selho Nacional de Desenvolvimento Cient´fico e Tecnologico ı do Brasil (CNPq) for the financial support. REFERENCES [1] J. F. van Staden, M. G. Mashamba, and R. I. Stefan, “Determination of the total acidity in soft drinks using potentiometric sequential injection titration,” Talanta, vol. 58, no. 6, pp. 1109–1114, 2002. [2] J. Marcos, A. R´os, and M. Valc´ rcel, “Automatic titrations ı a in unsegmented flow systems based on variable flow-rate patterns—part 1: principles and applications to acid-base titrations,” Analytica Chimica Acta, vol. 261, no. 1-2, pp. 489– 494, 1992. ´ [3] I. L. Garc´a, P. Vinas, N. Campillo, and M. H. Cordoba, “Linı ear flow gradients for automatic titrations,” Analytica Chimica Acta, vol. 308, no. 1–3, pp. 67–76, 1995. [4] P. B. Martelli, B. F. Reis, M. Korn, and J. L. F. C. Lima, “Automatic potentiometric titration in monosegmented flow system exploiting binary search,” Analytica Chimica Acta, vol. 387, no. 2, pp. 165–173, 1999. [5] A. P. S. Paim, C. M. N. V. Almeida, B. F. Reis, R. A. S. Lapa, E. A. G. Zagatto, and J. L. F. C. Lima, “Automatic potentiometric flow titration procedure for ascorbic acid determination in pharmaceutical formulations,” Journal of Pharmaceutical and Biomedical Analysis, vol. 28, no. 6, pp. 1221–1225, 2002. [6] R. S. Honorato, E. A. G. Zagatto, R. A. C. Lima, and M. C. U. ´ Araujo, “Prior assay as an approach to flow titrations. Spectrophotometric determination of iron in alloys and ores,” Analytica Chimica Acta, vol. 416, no. 2, pp. 231–237, 2000. [7] J. Marcos, A. R´os, and M. Valc´ rcel, “Automatic titrations ı a in unsegmented flow systems based on variable flow-rate patterns—part 2: complexometric and redox titrations,” Analytica Chimica Acta, vol. 261, no. 1-2, pp. 495–503, 1992. [8] H. du Plessis and J. F. van Staden, “Determination of sulphuric acid in process effluent streams using sequential injection titration,” Talanta, vol. 52, no. 1, pp. 83–90, 2000. [9] M. Korn, L. F. B. P. Gouveia, E. de Oliveira, and B. F. Reis, “Binary search in flow titration employing photometic endpoint detection,” Analytica Chimica Acta, vol. 313, no. 3, pp. 177–184, 1995. [10] A. J. C. Garcia and B. F. Reis, “Instrumentation and automated photometric titration procedure for total acidity determina- tion in red wine employing a multicommuted flow system,” , vol. 2006, Article ID 83247, 8 pages, 2006. F. R. P. Rocha, B. F. Reis, E. A. G. Zagatto, J. L. F. C. Lima, R. A. S. Lapa, and J. L. M. Santos, “Multicommutation in flow analysis: concepts, applications and trends,” Analytica Chimica Acta, vol. 468, no. 1, pp. 119–131, 2002. A. F. Lavorante, M. A. Feres, and B. F. Reis, “Multicommutation in flow analysis: a versatile tool for the development of the automatic analytical procedure focused on the reduction of reagent consumption,” Spectroscopy Letters, vol. 39, no. 6, pp. 631–650, 2006. ´ ´ E. Rodenas-Torralba, F. R. P. Rocha, B. F. Reis, A. MoralesRubio, and M. de La Guardia, “Evaluation of a multicommuted flow system for photometric environmental measurements,” , vol. 2006, Article ID 20384, 9 pages, 2006. F. R. P. Rocha and B. F. Reis, “A low-cost device for automatic photometric titrations,” Journal of Chemical Education, vol. 77, no. 2, pp. 258–261, 2000. [11] [12] [13] [14] http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Journal of Automated Methods and Management in Chemistry Hindawi Publishing Corporation

A Full Automatic Device for Sampling Small Solution Volumes in Photometric Titration Procedure Based on Multicommuted Flow System

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Copyright © 2007 Sivanildo S. Borges et al.
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Abstract

1 Centro 2 Centro de Energia Nuclear na Agricultura, Universidade de S˜ o Paulo, Avenida Centen´ rio 303, 13400-970 Piracicaba, SP, Brazil a a de Ciˆncias Exatas e Tecnol´gicas, Universidade Federal do Recˆncavo da Bahia, 44380-000 Cruz das Almas, BA, Brazil e o o Received 9 April 2007; Accepted 7 June 2007 In this work, an automatic device to deliver titrant solution into a titration chamber with the ability to determine the dispensed volume of solution, with good precision independent of both elapsed time and flow rate, is proposed. A glass tube maintained at the vertical position was employed as a container for the titrant solution. Electronic devices were coupled to the glass tube in order to control its filling with titrant solution, as well as the stepwise solution delivering into the titration chamber. The detection of the titration end point was performed employing a photometer designed using a green LED (λ = 545 nm) and a phototransistor. The titration flow system comprised three-way solenoid valves, which were assembled to allow that the steps comprising the solution container loading and the titration run were carried out automatically. The device for the solution volume determination was designed employing an infrared LED (λ = 930 nm) and a photodiode. When solution volume delivered from proposed device was within the range of 5 to 105 μl, a linear relationship (R = 0.999) between the delivered volumes and the generated potential difference was achieved. The usefulness of the proposed device was proved performing photometric titration of hydrochloric acid solution with a standardized sodium hydroxide solution and using phenolphthalein as an external indicator. The achieved results presented relative standard deviation of 1.5%. Copyright © 2007 Sivanildo S. Borges et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. INTRODUCTION Generally, in automatic titration procedure based on flow injection analysis process, the volume of the titrant solution delivered has been determined considering both flow rate and time interval elapsed while the titration was run [1–3]. In principle, it has been admitted that the flow rate was constant and the time interval was a very well-controllable variable [4, 5]. In these cases, peristaltic pump has been the device widely used to propel titrant solution [6–8]. Because pumping pulsation, due to peristaltic pump, could impair the precision of the delivered solution volume, a synchronization strategy has been implemented [4, 9]. Since peristaltic pump maintain a constant pulsation pattern, small volume of titrant solution, presenting good precision, could be delivered. Nevertheless, to accomplish this requirement, it is necessary to resort facilities comprising electronic and software [4, 9, 10]. Furthermore, the aging of the pumping tube could affect flow rate, thus this effect could become an error source. In this work, we intend to develop a device with ability to deliver small aliquots of titrant solution, determining also its volume with good precision and accuracy independent of both time and flow rate. The usefulness of the device will be demonstrated, coupling then to an automatic titration module based on multicommutation process [11, 12]. 2. 2.1. EXPERIMENTAL Solutions Purified water with electric conductivity less than 0.1 μS cm−1 was used throughout. An 89.2 ± 0.9 molL−1 HCl solution was prepared by dilution from a 1 molL−1 HCl solution. This solution was standardized by titration using an 88.7±0.8 molL−1 NaOH solution, which was previously standardized by titration using a potassium biphthalate solution and a 0.01% (w/v) phenolphthalein solution as indicator. 2.2. Apparatus The equipment set up comprised a Pentium III microcomputer furnished with an electronic interface card (PCL-711S, Advantech), an IPC-4 Ismatec peristaltic pump with Tygon PD Col Opt HC TR Pht LED BS B 30 cm TC CD LED1 (a) V1 TC AP (b) Tch V2 (c) Figure 1: View of the volume meter. (a) Detailed description of the device: TC = solution container, glass tube 30 cm long, 0.5 cm and 0.35 cm external and inner diameters, respectively; CD = solution inlet/outlet; B = floating device, polyethylene vial (transparent) with flat bottom, 25 mm long, 3.4 mm external diameter, 0.5 mm wall thickness; LED and LED1 = infrared light emitting diode (λ = 930 nm); Pht = phototransistor (Til78); Col = light beam collimator, metallic piece with dimension of 9 cm2 surface, 3.5 cm thickness, and central hole (1.0 mm diameter) for light transmission; PD = photodiode (Hamamatsu, S1337-1010BR). (b) Solution container hold; AP = acrylic plate with dimension of 15 × 20 × 1.5 cm; BS = brass cylinder, 30 cm long and 1.0 cm diameter; HC = glass tube holder, acrylic plate with dimension 15 × 10 × 1 cm. (c) Assembling view of the volume meter: TR = reservoir of titrant solution; V1 = pinch solenoid valve normally closed; V2 = three-way solenoid valve; Tch = titration chamber (14). Solid and doted lines into the valve (V2 ) symbol indicate the fluid pathway when valve was switched OFF and ON, respectively. pumping tubes, six three-way solenoid valves (161T031, Nresearch), one solenoid pinch valve normally closed (161P011, Nresearch), a homemade 12 V regulated power supply to feed the solenoid valves, a homemade electronic interface [13] to provide the potential difference and current intensity required to drive the solenoid valves, and a homemade photometric detector [14]. The control unit comprised one photodiode (Hamamatsu, S1337-1010BR), one phototransistor (Til78) wired as an optic switch, two infrared LED (λ = 930 nm), two operational amplifiers (OP07), one comparator device (LM339), and one transistor (BC547). The assays comprising the volume meter calibration and photometric titration were performed employing a software wrote in Quick BASIC 4.5. Flow lines were of Tygon tubing 0.56 mm inner diameter. 2.3. The volume meter description In Figure 1, it is shown a front view of the volume meter, where we can see that the device is coupled to the titrant solution reservoir (TR) through the solenoid valves V1 and V2 . The V2 was assembled to permit the container loading (TC) with titrant solution when valve V1 was switched ON. When the container was filled with titrant solution, the floating device (B) interrupted the infrared radiation beam of the optic switch (Opt). When the electronic interface showed in Figure 2 sensed the interruption of the radiation beam, it generated the control signal to switch OFF valve V2 in order to stop the stream of the titrant solution. 12 V 1k LED B 10 k 4 Opt 5V Pht1 5 + −1 4 LM339 10 k D0 Pw V1 12 V TC 20 k 12 V Ens Figure 2: Diagram of the device to control the filling of the titrant solution container. Opt = optic switcher, LED = infrared emitting diode (930 nm), Pht = phototransistor (Til78), Pw = power driving device (ULN2803), D0 = Pw first input line, V1 = pinch solenoid valve normally closed, Ens = control enabling line. The optic switch (Opt) comprising an infrared radiation emitting diode (λ = 930 nm) and a phototransistor (Til78), which was attached in a metallic piece (5 × 5 × 0.4 cm) with a central lead hole to permit the inserting of the solution container (TC), thus allowing that the container was positioned between the phototransistor (Pht) and the infrared LED. A hole with a diameter of 1.0 mm was drilled at the orthogonal position to the lead hole in order to permit that the infrared Sivanildo S. Borges et al. Table 1: Steps sequence of the titration procedure. Step 0 1 2 3 4 5 6 7 8 9 10 11 ∗ V1 0 1 0 0 0 0 0 0 0 0 0 0 V2 0 0 0 0 0 0 0 0 0 0 1 0 V3 0 0 0 0 0 1 0 0 0 1 0 0 ∗∗ V4 0 0 0 0 0 1 0 0 0 1 0 0 V5 0 0 0 1 0 0 0 1 0 0 0 0 V6 0 0 0 1 0 0 0 0 1 0 0 0 ∗∗∗ V7 0 0 0 0 1 0 1 0 0 0 0 0 D0 Pw 0 1 0 0 0 0 0 0 0 0 0 0 Time (s) — — — 20 15 20 20 sit∗∗∗ 2 8 — — Description Standby Fill titrant container Standby Fill flow line S and In∗ Empting titration chamber Washing titration chamber∗∗ Empting titration chamber∗∗ Sample inserting time Indicator insertion Carrier solution insertion Start titration End titration S = sample, In = indicator solution; steps that were repeated twice; sit = value defined when the software was run. beam attained the phototransistor (Pht) after it crosses the titrant solution container (TC). As it is depicted in Figure 1, an infrared radiation emitting diode (LED1) was installed at the bottom of the titrant solution container (TC), thus the radiation beam emitted by this LED was directed towards the photodiode (PD) through the liquid column maintained inside of the container. The liquid column behaves as a wave guide and it was observed that its length affected the intensity of the infrared radiation beam that reaches the photodiode (PD). The volume meter was developed exploiting this effect. 2.4. The volume meter calibration The filling of titrant solution container (TC) was controlled by mean of the electronic interface showed in Figure 2. Prior to load the container with titration solution, the system was adjusted following the steps summarized in Table 1. Maintaining the titrant solution container empty, the signal generated by the optic switch (Opt) was 3.8 V that was applied to the no inverting input of the comparator device (LM339, pin 5). Reference signal applied to the comparator input (pin 4) was adjusted to 3.5 V turning the variable resistor (20 kΩ) wired to it. Under this condition, the output of the comparator device (pin 2) was at a high-state condition and the power-driving device (Pw) was maintained deactivate, while the control enabling line (Ens) was at low level (0 V). When the software was run, the microcomputer sent a control signal (TTL high level) through PCL711 interface card to enable the control line (Ens, Figure 2). Under this condition, the input line (D0 ) of the power-driving device (Pw) was enabled to switch ON valve V1 , thus the titrant solution flowed from its vessel (TR, Figure 1) by the gravity acceleration action to fill the titrant container (TC) with titrant solution. While the liquid column increased into the container, the floating device (B) was displaced toward the top. When it crossed the light beam of the optic switch (Opt), the signal sent to the comparator input (pin 5) fall lower than 3.0 V. Under this condition, the output signal of the comparator device (pin 2) was drove to the low-state condi- tion (0 V), thus disabling the line input (D0 ) of the powerdriving device (Pw), which switched OFF valve V1 in order to stop the stream of titrant solution. The light emitting diode (LED1) installed in the container bottom (TC, Figure 1) was switched OFF by turning the variable resistor wired to the base of the transistor (Tr1, Figure 3). The signal output (So) of the operational amplifier (OA2) was adjusted to 0 V by turning the variable resistor (20 kΩ) wired to the no inverting input of this operational amplifier. Afterwards, the emission intensity of the LED1 was raised up to the output signal (So) attained 2000 mV. This was done turning the variable resistor coupled to the base of the transistor (Tr1). The flow diagram of the titration system is shown in Figure 4. In this configuration, all valves are switched OFF, thus all solutions propelled by the peristaltic pump (PP) are directed towards their storing vessels. When valve V2 was switched ON, the titrant solution flowed through it. Aiming to find the relationship between the solution volumes delivered from the container (TC) and the output signal (So) generated by photodiode (Figure 3), a set of assays was carried out. The microcomputer sent, through the output port of the PCL711S interface card, a control signal to switch ON valve V2 . While solution flowed from the container (TC), the microcomputer read the variation of the signal (So) through the analog input of the PCL711S interface card. When signal variation attained a preset value (Vs), valve V2 was switched OFF in order to stop the solution stream, and the delivered volume of solution was measured. Assays were performed programming potentials difference ranging from 50 up to 800 mV. After calibration stage, the valve V2 was maintained switched ON during a time interval of 2 minutes to empty the titrant solution container. After calibration, a set of titration assays was carried out to demonstrate the usefulness of the proposed volume meter, which was implemented using the flow system showed in Figure 4, which was designed based on multicommutation process [10–12]. Titration chamber (Tch) and photometer detector (not showed) were similar to those employed in previous work [14]. 0.47 μF 10 M 12 V 5k 20 k 270 Tr1 LED1 PD 12 V 2 − 0.47 μF 470 k C1 12 V 100 k 2 C3 10 k S0 OA1 + 3 4 C2 −12 V − 7 6 OA2 + 3 4 C4 −12 V 100 k 20 k +12 V −12 V Figure 3: Electronic diagram of the interface to monitor the titrant solution into the container. Tr1 = transistor (BC547), LED1 = light emitting diode (930 nm), PD = photodiode (Hamamatsu, S1337-1010BR), OA1 e OA2 = operational amplifiers (OP07), C1, C2, C3, and C4 = 1 μF tantalum capacitors, So = signal output. Ri Rc PP In V3 V4 Cs V5 Rs S V7 V6 VM T Tch V2 PC TR V1 Table 2: Signal generated as function of the delivered water volume. Signal (mV) 56 100 140 165 234 273 318 372 463 559 791 Volume (μL) 5.7 10.3 14.9 19.0 28.0 32.6 38.4 46.4 58.7 72.5 103.9 Table 3: Comparison between the solution volumes measured and the preset values, results are average of three measurements. Figure 4: Diagram of the flow system. V1 , = pinch solenoid valve, V2 , V3 , V4 , V5 , V6 , and V7 = three way solenoid valves, S = sample; Cs = carrier solution, water, In = indicator, 0.01% (w/v) phenolphthalein solution, Rs, Rc, and Ri = solutions (S, Cs, In) circulation towards their storing vessels, respectively; W = waste, PP = peristaltic pump, T = titrant solution, 88.7 ± 0.8 molL−1 NaOH, Tch = titration chamber, TR = titrant solution reservoir, VM = volume meter (Figure 1), PC = microcomputer. Measured volume (μL)∗ 17.93 ± 0.06 29.40 ± 0.05 58.6 ± 0.7 76.7 ± 0.3 100.5 ± 0.6 ∗ Preset volume (μL) 17.7 ± 0.2 29.3 ± 0.3 58.8 ± 0.5 77.7 ± 0.4 99.6 ± 0.7 Values obtained weighting the delivered volume of water and considering the water density at 25◦ C. As it is depicted in Table 1, in the standby condition all valves are switched OFF, thus all solutions are pumped back to their storing vessels (Figure 4). When the software was started to carry out a titration run, the microcomputer sent a control signal (TTL high level) through the enabling line (Ens, Figure 2) to enable the power-driving device (Pw, Figure 2). Under this condition, valve V1 was switched ON to fill the container (TC) with titrant solution. This step was done as it was described in previous section. Afterwards, valves V5 and V6 were switched ON during a time interval of 20 seconds (step 3) to fill the flow lines up to the titration chamber (Tch). Afterwards, valve V7 was switched ON during a time interval of 15 seconds (step 4) to empty the titration chamber. The washing of the titration chamber with carrier solution comprised the steps 5 and 6 (Table 1), which were repeated twice to assure good cleaning. Following the working sequence showed in Table 1 (steps 7, 8), valves V5 and V6 were sequentially switched ON during preset time intervals to insert into the titration chamber aliquots of sample solution (S) and of indicator solution (In), Sivanildo S. Borges et al. Table 4: Comparison of the titration results, results are average of three consecutive titration run that were performed using a 88.7 ± 0.8 molL−1 NaOH standardized solution. Sample (HCl) 1 2 3 4 5 6 Sample volume (μL) 43 57 71 85 100 115 Actual HCl concentration (molL−1 ) 89.2 ± 0.9 89.2 ± 0.9 89.2 ± 0.9 89.2 ± 0.9 89.2 ± 0.9 89.2 ± 0.9 Found HCl concentration (molL−1 ) 89.5 ± 0.6 88.5 ± 0.9 89.1 ± 1.5 89.8 ± 0.5 88 ± 1 88 ± 1 Difference (%) −0.3 0.8 0.1 −0.7 1.3 1.3 respectively. The time interval to maintain valve V6 switched ON was settled at 2.0 seconds, while time for valve V5 was varied from 3.0 up to 8.0 seconds. Afterwards, valves V3 and V4 were switched ON during a time interval of 8.0 to insert 800 μl of the carrier solution into the titration chamber. As it is shown in Table 1 (step 10), valve V2 was switched ON to permit that the titrant solution flowed continuously by the gravity acceleration action toward the titration chamber (Tch). The monitoring of the signal generated by the photometer was performed by the microcomputer through the analog input of the PCL711S interface card. When a quick transition of the generated signal occurred, the microcomputer sent a control signal through the enabling line (Ens, Figure 2) to switch OFF valve V2 in order to stop the stream of the titration solution. This signal changing indicated that the stoichiometric condition was attained [14]. Afterwards, the microcomputer read the signal (S0 ) generated by the photodiode (PD) of the volume meter (Figure 3) that was saved as an ASCII file. The volume of the titrant solution used to find the end of titration was calculated using this measurement. When the signal (S0 ) surpassed a preset threshold value, which was related to a delivered solution volume of the titrant solution about 85 μl, the microcomputer halted the stream of the titrant solution and saved the signal value related with the solution volume that was used at that moment. Afterwards, the volume meter-filling step was carried out again and after that the titration run was reestablished in order to find the end of titration. 3. RESULTS AND DISCUSSIONS Volume meter calibration Intending to find the relationship between the volume of the solution delivered and the potential difference generated by the photodiode (PD), a set of assays was carried out yielding the results showed in Table 2. Processing these data, we found the following linear relationship: ΔE(mV) = −25.7 − 7.4 v(μL), (R = 0.999). Aiming to confirm the linear relationship, experiments were carried out at several days. The assays were done settling different values of potential difference and no significant difference was observed. Every day prior to begin the first titration run, the calibration stage was accomplished in order to find the parameters related to the linear relationship, which were incorporated in the control software to permit that the volume of titrant solution was calculated when titration run was ended. Intending to prove the ability of the device to deliver a preset solution volume, a set of experiments was performed using distilled water and results are showed in Table 3. Processing these data, a linear relationship presenting a slope of 0.999 and an intercept tending to 0.0 was achieved. These results indicated that the system was able to determine the solution volume processing the potential difference related to liquid column height. Furthermore, the precision of the delivered volumes was better than 1.0% (n = 10) which was confirmed repeating the experiments maintaining the preset values. 3.3. Automatic titration 3.1. General comments The volume meter working principle was based on the attenuation of the radiation beam intensity, which was affected by the height of the liquid column inserted between the electromagnetic radiation source (LED1, Figure 1) and the photodiode (PD). The value of the potential difference generated by the photodiode decreased when the gap between the liquid column top and the photodiode (PD) increased. Previous assays performed using LEDs with wavelength of 470 nm (blue), 650 nm (red), and 930 nm (infrared) showed that better linear range could be obtained with the infrared LED. In this sense, the results commented below were obtained employing this component. Aiming to demonstrate the usefulness of the proposed volume meter device, photometric titration of hydrochloric acid with sodium hydroxide solution was performed yielding the results showed in Table 4. The volumes of the HCl solution aliquots were varied from 43 up to 115 μL. As we can see the concentration of the HCl solution found is closed to expected values. In the assays labeled as 5 and 6 the volumes of the HCl solution aliquots used were 100 and 115 μL, respectively, thus the solution container (TC, Figure 1) was filled twice. Analyzing the results, we can see, that in both cases accuracy and precision were similar to the other ones showed in Table 4. 4. CONCLUSIONS The performance of the proposed volume meter shows that it can be used to deliver small volume with good precision 6 independent of the flow rate and the time interval. The instrumental arrangement is very simple and easy to be replicated in laboratory with a few little electronic facilities. The volume meter was successfully applied in the determination of the titrant solution volume in photometric titration procedure of hydrochloric acid with sodium hydroxide solution. Albeit, the operational work range was between 5 and 105 μL, the appropriated combination of software and hardware were able to refill the titrant solution container while the titration run was in course. The volume meter device presented a very good longterm stability, which was ascertained by working several days and no significant variation concerning to linear response range, precision, and accuracy was observed. ACKNOWLEDGMENTS ` Authors gratefully acknowledge the Fundacao de Amparo a ¸˜ Pesquisa do Estado de S˜o Paulo (FAPESP) and the Cona ´ selho Nacional de Desenvolvimento Cient´fico e Tecnologico ı do Brasil (CNPq) for the financial support. REFERENCES [1] J. F. van Staden, M. G. Mashamba, and R. I. 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Journal

Journal of Automated Methods and Management in ChemistryHindawi Publishing Corporation

Published: Aug 26, 2007

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