- Open Access
- Total Downloads : 226
- Authors : Shantaram L. Bonde, Suchita P. Bhangale, Pravin K. Bhadane
- Paper ID : IJERTV3IS090891
- Volume & Issue : Volume 03, Issue 09 (September 2014)
- Published (First Online): 27-09-2014
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Investigation of Some Electronic Properties of Combined pH Electrode
Shantaram L. Bonde1, 1Department of Chemistry Nowrosjee Wadia College Pune,India-411001
Suchita P. Bhangale2 and Pravin K. Bhadane2 2Department of Electronics
Nowrosjee Wadia College Pune,India-411001.
Abstract Some electronic properties of combined pH electrode have been investigated with the help of electronic circuits. Electrode-electrolyte resistance has been measured by half deflection method and its value depends on the thickness of glass. The bulk resistance of test solution, internal solution of glass and reference electrodes have been measured by AC Wheatstones bridge and they are dependent on ionic concentration. The capacitance of glass electrode has been measured by de Sautys bridge. The impedance of double screened co-axial cable has measured by LCR meter. The measured values of resistance and capacitance are matching with the desired values. Present study is useful to the electronic engineers for designing of preamplifier section of pH meter.
Keywordscombined pH electrode, electrode-electrolyte resistance, AC Wheatstones bridge, de Sautys bridge.
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INTRODUCTION
pH measurement is generally done with the use of a combination electrode. The combination electrode is an electrode system formed by a glass half-cell which works as measuring electrode and reference half- cell. A potential develops on the membrane surface when a pH electrode comes in contact with a sample and its value varies with the pH of the sample [1]. The voltage signal produced by the pH electrode is a very small, high impedance signal. Due to this reason, the voltmeter is not directly connected to the pH electrode. An interface of amplifier with high input impedance is required between the electrode and voltmeter. With the age of glass electrode, its resistance changes. Generally it increases due to chemical deposition and deformation due to thermal effect. This resistance change alters the electrode potential. For this cause, electrode should be calibrated regularly. The resistance of electrode depends on the type of material used for making the glass balloon.
The balloon of pH electrode is made from a special glass composed of alkali metal ions [2-4]. The alkali metal ions of the glass and the hydrogen ions in solution undergo an
concentration of solutions. The response time of pH measurement depends on the capacitance.
The potential of the reference portion is produced by the internal element in contact with the reference fill solution. The potential at glass electrode is measured with reference to the potential of reference electrode. In order to measure the correct potential due to test solution, the potential of reference electrode should be constant [5]. For this reason, the fill solution should contain constant number of ions. The saturated solution of salt, such as KCl, has more ions and less resistance of the order of 2000 .
The present work deals with the measurement of resistance and capacitance of combined pH electrode. The resistance of glass and solution were measured by half deflection method and AC Wheatstones bridge respectively. The capacitance of glass was measured by the de Sautys bridge method. The rest of article is organized as follows: in section II electrical equivalent circuit of combined pH electrode is discussed. The design of electronic circuits, their description and results are discussed in section III. Finally, the conclusion and the future scope of present work are discussed in section IV.
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METHOD
In the present work, electronic parameters of combined electrode have been measured by designing the electronic circuits. Figure 1 shows the combined electrode and it also shows the corresponding equivalent electronic components. The balloon of glass electrode forms the electrode-electrolyte interface and it is equivalent to the parallel combination of resistor (Rg) of glass and capacitor (Cg) with glass as dielectric. The internal and external ionic solutions form the plates of parallel plate capacitor. The resistance of internal solution (Rint) is in series with Rg and Ag/AgCl wire. The Rg and Cg are given by [6],
ion exchange reaction generating a potential difference.
Electronically, the ion exchange is equivalent to the leakage of charge through the glass membrane. The glass membrane
Rg =
× d
B , Cg =
0 × k × A d
forms the solid dielectric medium of non-polar capacitor. The internal ionic buffer solution and the external test solution form the plates of capacitor. The value of capacitance depends on the thickness of glass membrane and the ionic
Where, =specific resistance, d= thickness, B= cross-
sectional area, 0= permittivity of free space, k=dielectric constant, A=surface area of balloon.
The resistance of glass and ionic solutions cannot be measured by electronic ohm meter. This is due to non- conducting behavior of glass and the nature of charge transport in the ionic solution. Special methods are required to measure them and they are discussed in the next section.
Fig.1 shows the electrical equivalent circuits of glass electrode, reference electrode, test solution and the co-axial cable. The reference electrode is filled with saturated solution with resistance (Rr). The resistance of liquid junction is ignored because it is negligible as compared to Rr.
The potential produced by the electrode is very small. The amplifier with low bias current is required to increase the strength of electrode signal. The signal carrying wire should have minimum resistance (Rwi). The screen of co-axial cable is used to carry the return signal. This outer layer should have less resistance (Rwo). The insulating PVC cover of the inner wire forms the dielectric of cylindrical capacitor (Cins). There is possibility of leakage of charge through the insulating
-
A known variable resistor (Rk) is connected in series with Rg and by varying Rk, the voltage across Rg is reduced to ½ Vfd, as shown in fig 2(b).
The voltage across Rg can be calculated by using potential divider formula,
coating of wire. The capacitance due to insulation should be minimum, and it is possible by use of thick insulating cover.
vRg =
vfd
=
2 Rg
Rg
k
+ R vin
Further, value of Rg can be obtained as,
vfd × Rk
2v
Rg =
in
vfd
Fig.1: Electrical equivalent circuit of combined pH electrode
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ELECTRONIC CIRCUIT DESIGN AND
RESULTS
-
Measurements of Resistance
-
Measurement of Rg: It is the resistance due to charge transferred through glass medium and it cannot be measured by dc Ohm-meter. The charge transferred through glass is negligible and due to this, Ohm-meter is not suitable
-
At half deflection position, resistance Rk equals to Rg. The value of Rk can be obtained by using Ohm-meter.
Above method has been used to measure the resistance Rg of glass electrode. The measured Rg of new and old glass electrodes are 400 M and 420 M respectively.
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-
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Measurement of Bulk Resistance (Rext) of Solution and Resistance (Rint) of Internal Buffer Solution
These resistances are due to the ionic charge transport in solution. They can be measured with the use of AC Wheatstones bridge as shown in fig. 3.
The resistor R3 is varied to balance the bridge. The resistances Rint or RExt can be obtained from bridge balance condition,
for the measurement of Rg. In the present work we have sed
the half deflection method which is based on the measurement of potential difference (PD).
Rint
R1 × R2
=
R3
Half deflection method: Rg can be measured in following three steps.
a) Voltage across Rg is measured and it is called full deflection (Vfd) as shown in figure 2(a).
Where R1 and R2 are fixed resistors and R3 is variable resistor used for balancing the bridge.
Above method has been used to measure the resistance of test (RExt) and internal buffer (Rint) solutions. The RExt of 0.05 M Potassium Hydrogen Pthalate and Rint of 0.1M HCl are 9 K and 5 K respectively.
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Measurement of Capacitance (Cg)
The balloon of glass forms the dielectrics of capacitor glass and it is measured by de Sautys bridge method as shown in figure 4.
If bridge is balanced then Cg is given by,
R2 × Ck
R
Cg =
1
REFERENCES
-
G. R. Chatwal, S. K. Anand, Instrumental methods of chemical analysis, Himalaya publishing house, 5th Edn, 2008.
-
R.A. Weeks, The structure of glass: past, present, and prescient, Volume 73, Issues 13, Pages 273284, August 1985.
-
F.G. K. Baucke, The glass electrode-applied electrochemistry of glass surfaces, Journal of Non-Crystalline Solids Volume 73, Issues 13, Pages 215231, August 1985.
-
M.M. Shultz, Chemistry of glass, Journal of Non-Crystalline Solids Volume 73, Issues 13, Pages 91101, August 1985.
-
Skoog, D. M. West, F. J. Holler & S. R. Crouch, Fundamentals of Analytical Chemistry, 8th Edn, Thomson-Brooks/Cole, 2004
-
Paul Horowitz and Winfield Hill, The art of Electronics, 2nd Edn., Cambridge University Press, 1989.
ABOUT AUTHORS:
Above method has been used to measure the capacitance Cg of glass. The Cg of new and used combined electrodes are 60pF and 58 pF respectively. The results of measurements of electrical properties of combined pH electrode are summarized in Table I.
Dr. Shantaram L. Bonde is Principal at Nowrosjee Wadia College, Pune (India). He is author of twenty research papers. His research interests are in the field of physical and analytical chemistry.
Prof. (Mrs.) Suchita P. Bhangale is working as Assistant Professor of Electronics at Nowrosjee Wadia College, Pune (India). She is pursuing her Ph.D. work in the field of analytical instrumentation.
Dr. Pravin K. Bhadane is Head of the Electronics Department at Nowrosjee Wadia College, Pune (India). He is author of sixteen research papers. His research interest
is in the field of analytical instrumentation.
TABLE I. Electrical properties of combined pH electrode
Sr.
No.
Property
Combined pH electrode
New
Old
1
Resistance of glass (Rg)
400M
420M
2
Capacitance due to glass balloon (Cg)
60pF
58pF
3
Resistance of 0.1 M HCl (Rint)
5K
5.4K
4
Resistance of saturated KCl (Rr)
2K
2.2K
5
Resistance of pH 4 solution (Rext)
9K
9.8K
6
Resistance of inner conductor of
coaxial cable (Rwi)
0.1 /m
0.11 /m
7
Resistance of screen of coaxial cable
(Rwo)
0.12 /m
0.13 /m
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CONCLUSIONS AND FUTURE SCOPE Resistance and capacitance of combined electrode play
significant role in the measurement of potential. The value of resistance is very high and it changes due to the chemical deposition. The glass electrode is more sensitive to pH measurement, if its resistance is low. Capacitance of glass electrode depends upon thickness of glass and its composition. For better sensitivity capacitance value should be high and it can be achieved by use of thin glass. The measurement of resistance and capacitance values of combined pH electrodes are necessary for the design of an amplifier circuit of pH meter.
In the present work, prototype electronic circuits were designed using ordinary readily available components. They are manually operated circuits and give good estimate of the parameters of pH electrode. In future, our plan is to develop automatic system using special components for the measurement of parameters.