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 (lambda=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 (lambda=930 nm) and a photodiode. When solution volume delivered from proposed device was within the range of 5 to 105 mul, 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%.
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 (lambda=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 (lambda=930 nm) and a photodiode. When solution volume delivered from proposed device was within the range of 5 to 105 mul, 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%.
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. EXPERIMENTAL
2.1. Solutions
Purified water with electric conductivity less than 0.1 μS cm−1 was used throughout. An molL−1 HCl solution was prepared by
dilution from a 1 molL−1 HCl solution. This solution was standardized
by titration using an 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 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 ( 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.
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 ( nm); Pht = phototransistor (Til78); Col = light beam collimator, metallic piece with dimension of 9 cm 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 cm; BS = brass cylinder,
30 cm long and 1.0 cm diameter; HC = glass tube
holder, acrylic plate with dimension 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.
Figure 2
Diagram of the device to control the filling of the titrant solution
container. Opt = opticswitcher, 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 ( nm) and a phototransistor (Til78), which was attached
in a metallic piece ( 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
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 condition (0 V), thus disabling
the line input (D0) of the power-driving 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).
Table 1
Steps sequence of the titration procedure.
Step
V1
V2
V3
V4
V5
V6
V7
D0 Pw
Time (s)
Description
0
0
0
0
0
0
0
0
0
—
Standby
1
1
0
0
0
0
0
0
1
—
Fill titrant container
2
0
0
0
0
0
0
0
0
—
Standby
3
0
0
0
0
1
1
0
0
20
Fill flow line S and In*
4
0
0
0
0
0
0
1
0
15
Empting titration chamber
5
0
0
1
1
0
0
0
0
20
Washing titration chamber**
6
0
0
0
0
0
0
1
0
20
Empting titration chamber**
7
0
0
0
0
1
0
0
0
sit***
Sample inserting time
8
0
0
0
0
0
1
0
0
2
Indicator insertion
9
0
0
1
1
0
0
0
0
8
Carrier solution insertion
10
0
1
0
0
0
0
0
0
—
Start titration
11
0
0
0
0
0
0
0
0
—
End titration
*S = sample, In = indicator solution; **steps that were repeated twice; ***sit = value defined when the software was run.
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, S0 = signal output.
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.
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, molL−1 NaOH, Tch = titration chamber, TR = titrant solution reservoir, VM = volume meter (Figure 1), PC = microcomputer.
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].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),
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
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.
3.2. 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), (). 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.
Table 2
Signal generated as function of the delivered water volume.
Signal (mV)
Volume (μL)
56
5.7
100
10.3
140
14.9
165
19.0
234
28.0
273
32.6
318
38.4
372
46.4
463
58.7
559
72.5
791
103.9
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% () which was confirmed repeating the experiments
maintaining the preset values.
Table 3
Comparison between the solution volumes measured and the preset values,
results are average of three measurements.
Measured volume (μL)*
Preset volume (μL)
17.93±0.06
17.7±0.2
29.40±0.05
29.3±0.3
58.6±0.7
58.8±0.5
76.7±0.3
77.7±0.4
100.5±0.6
99.6±0.7
*Values obtained weighting the delivered volume of water and
considering the water density at 25°C.
3.3. Automatic titration
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.
Table 4
Comparison of the titration results, results are average of three consecutive titration run that were performed using a molL−1 NaOH standardized solution.
Sample (HCl)
Sample volume (μL)
Actual HCl concentration (molL−1)
Found HCl concentration (molL−1)
Difference (%)
1
43
89.2±0.9
89.5±0.6
−0.3
2
57
89.2±0.9
88.5±0.9
0.8
3
71
89.2±0.9
89.1±1.5
0.1
4
85
89.2±0.9
89.8±0.5
−0.7
5
100
89.2±0.9
88±1
1.3
6
115
89.2±0.9
88±1
1.3
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
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
long-term stability, which was ascertained by working several days
and no significant variation concerning to linear response range,
precision, and accuracy was observed.
Authors: Ana Paula S Paim; Cristina M N V Almeida; Boaventura F Reis; Rui A S Lapa; Elias A G Zagatto; José L F Costa Lima Journal: J Pharm Biomed Anal Date: 2002-06-15 Impact factor: 3.935
Authors: Eva Ródenas-Torralba; Fábio R P Rocha; Boaventura F Reis; Angel Morales-Rubio; Miguel de la Guardia Journal: J Autom Methods Manag Chem Date: 2006