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International Journal of Electrochemistry
Volume 2011 (2011), Article ID 670513, 5 pages
Research Article

Cyclic Voltammetry and Impedance Spectroscopy Behavior Studies of Polyterthiophene Modified Electrode

Laboratoire d'Electrochimie et Matériaux, Département de Génie des Procédés, Faculté de Technologie, Université Ferhat Abbas, 19000 Sétif, Algeria

Received 10 May 2011; Accepted 20 June 2011

Academic Editor: José H. Zagal

Copyright © 2011 Naima Maouche and Belkacem Nessark. 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.


We present in this work a study of the electrochemical behaviour of terthiophene and its corresponding polymer, which is obtained electrochemically as a film by cyclic voltammetry (CV) on platinum electrode. The analysis focuses essentially on the effect of two solvents acetonitrile and dichloromethane on the electrochemical behaviour of the obtained polymer. The electrochemical behavior of this material was investigated by cyclic voltammetry and electrochemical impedance spectroscopy (EIS). The voltammograms show that the film of polyterthiophene can oxide and reduce in two solutions; in acetonitrile, the oxidation current intensity is more important than in dichloromethane. The impedance plots show the semicircle which is characteristic of charge-transfer resistance at the electrode/polymer interface at high frequency and the diffusion process at low frequency.

1. Introduction

As other conjugated conducting polymers, polythiophene and its oligomers can be polymerized from their monomers in solutions by electrochemical methods. The electrochemical synthesis is advantageous method: polymers are formed in the doped state; films generally possess interesting electrochemical and good semiconductor properties [1] and relatively good stability in air for both the neutral and oxidised states [27].

The mechanism of the electropolymerisation of conducting polymers and polyheterocycles occurred by the coupling via α-α bonding of monomer radical cation after its oxidation at the electrode, and the protons are removed from dihydrodication leading to neutral species [810]. As the dimer is more easily oxidized than the monomer, it is immediately oxidized. The chain elongation occurs by the addition of new monomer radical cation leading to polymerization and forms the insoluble polymeric species, which subsequently deposits onto the electrode [11].

Conducting polymer-modified electrodes have been widely investigated because of their potential application in areas such as electrocatalysis [12, 13], sensors [14, 15], corrosion [1618], batteries [19, 20], electronic displays, and devices [2124].

In our previous work [25], we have studied the role of P3T in corrosion of stainless steel; the results were important and show effectively that the film of P3T will decrease the corrosion rate. In this paper, we are interested in performing an electrochemical characterisation of P3T films electrochemically synthesized, in two organic solvents: acetonitrile (CH3CN) and dichloromethane (CH2Cl2), at platinum substrates. We want to show how the medium of the analysis is depending upon the electrochemical and electronic behaviour of the formed films.

2. Experimental

The solvents acetonitrile and dichloromethane, Aldrich pure products for analysis, were used without further purification. Terthiophene (3T) was purchased from Aldrich (98%), and it was used as received; the supporting electrolyte salt tetrabutylammonium perchlorate (TBAP) was purchased from Fluka; this salt was first dried at a temperature of 80°C for 4 h before its use for the preparation of solution.

Electrochemical measurements were carried out on potentiostat/galvanostat Voltalab 40 interfaced with a PC under Voltamaster 4 software, in a three-electrode cell consisting of: platinum working electrode (diameter 2 mm), which was served as a substrate for the deposition of polyterthiophene (P3T), wire platinum as auxiliary electrode, and a saturated calomel electrode (SCE) as reference.

Electrochemical impedance spectroscopy measurements were performed using an impedancemeter Z-computer TACUSSEL controlled by microcomputer HEWLETT-PACKARD. The assembly is coupled to a plotter and a printer. The impedance spectra were recorded in the frequency range 105 Hz–10−3 Hz with an amplitude of 10 mV, in three-electrode electrochemical cell. All experiments were carried out at room temperature.

Before the electrochemical deposition of polyterthiophene for each experiment, the working electrode was polished by 0.03 μm alumina slurry and rinsed with distilled water and acetone for the removal of excess 3T monomer.

3. Results and Discussion

3.1. Electropolymerisation of Terthiophene

Figure 1 shows the cyclic voltammograms (12th cycles) 10−2 M of 3T dissolved in CH3CN solution containing 0.1 M of TBAP supporting electrolyte at Pt electrode, in potential scans between 0 and 1.2 V versus SCE with scan rate of 50 mV/s. The first scan shows that the terthiophene is oxidized to its radical cation at potential of +1.07 V [26], and immediately the polymer was formed. In the reverse cathodic scan, a polymer reduction peak was observed at a potential of 0.70 V. The current of the oxidative peak progressively increases with the number of cycles indicating the formation and the growth of conducting polymer film and suggests that there is systematic increase in the electrode area as a result of the actual deposition of P3T [27, 28]. The films formed are stable on the electrode and can easily be transferred to an electrolyte solution in absence of monomer.

Figure 1: Electrochemical polymerization of 3T (a) 1rst cycle, repetitive cycling (b) in a solution of TBAP 0.1 M in acetonitrile, scan rate 50 mV/s.
3.2. Cyclic Voltammetry Characterisation

After polymerization, the working electrode was extracted from the cell, rinsed with acetone, and dried with a gentle nitrogen flux, then analysed by cyclic voltammetry and impedance spectroscopy in the monomer-free solution of CH3CN/TBAP and CH2Cl2/TBAP, respectively.

Figure 2 shows the cyclic voltammograms of P3T film in CH3CN/0.1 M of TBAP solution, recorded at different voltage scan rates 10 (a), 20 (b), 50 (c), and 100 mV/s.

Figure 2: Cyclic voltammograms corresponding to P3T film in a solution of CH3CN/TBAP 0.1 M, recording for different scan rates: (a) 10, (b) 20, (c) 50, and (d) 100 mV/s.

The voltammogram recorded at scan rate of 10 mV/s (inset of Figure 2) shows a single oxidation peak located at 1.06 V and two reduction processes, one at around 0.96 V and the other less intense at 0.74 V. However, we observe that, except for their oxidation potential, which depends on the chain length of the oligomer, the shape of voltammetric curves is similar, and the same behavior was also observed with different thiophene oligomers [2933].

The film formed on the platinum electrode is electrochemically active and shows a reversible change of colour, a red in the oxidation state and blue in the reduction one. This phenomenon of P3T based on reversibly coloured electrochromic materials has become the subject of many interest applications. The electrochemical stability of the film was shown by repetitive voltammograms which remain essentially stable with cycling, and no evolution of the oxidation or the reduction current is observed. The stability of the oligothiophenes in air is already discussed in the literature [3, 34], and it is one of the most important properties of polyoligothiophenes.

The film of P3T was furthermore studied in CH2Cl2/TBAP in absence of monomer. The corresponding voltamperograms are presented in Figure 3. Also it can be shown that the film can oxide and reduce, and practically the same allure of voltammograms is obtained; however, the electroactivity of the film in CH3CN was more defined and has a high oxidation current.

Figure 3: Cyclic voltammograms corresponding to P3T film in a 0.1 M solution of TBAP in dichloromethane recording for different scan rates; (a) 10, (b) 20, (c) 50, and (d) 100 mV/s.

The voltammogram obtained here do not show clearly the anodic peaks except in the return scan; we observe a peak at 0.51 V attributable to the reduction of the film deposited on the electrode. So, contrary to the analysis realized in acetonitrile medium, in dichloromethane, the oxidation peak is poorly defined and is concealed, probably because of strong participation of capacitive current. The current intensity of the anodic and cathodic peak increases with scan rate. Also, the waves and the oxidation peaks do not appear when curves are recorded with high scan rates (  mV/s), this is the result of the participation of a large capacitive current which becomes important as the scan rate increases. The difference (ΔEp) between the oxidation potential and the reduction one increases with the scan rates. The proportionality of the peak intensity to the scan rates suggests that the oxidation of electroactive polymer obtained on the electrode surface is limited by a diffusional process [30].

These results suggest that the thickness of the film is smaller than the diffusion layer thickness of counteranions on the cyclic voltammetric time scale used here, which must diffuse in and out during the doping and dedoping processes. The oxidation peaks shifted to more positive potential at scan rates increase; this suggests that as explained in reference [33] (i) the electron transfer from the electrode to the polymer film may be slow; (ii) the rate of electron transfer may be controlled by the diffusion of counter ions at a scan rate faster than 10 mV/s; and/or (iii) the ohmic potential drop across the film may be significant.

3.3. Electrochemical Impedance Spectroscopy Characterization

Figure 4 gives the Nyquist plots of the electrodes coated by P3T/Pt, obtained in solution of CH3CN/TBAP 0.1 M (Figure 4(a)) and in CH2Cl2/TBAP 0.1 M (Figure 4(b)). It can be seen that the two impedance curves have a semicircle in the high-frequency region for each medium, and the semicircle in acetonitrile is smaller than that in dichloromethane. The high-frequency part gives electrolyte resistance (Re) by the distance from the original value, and the width of the semicircle gives the estimated impedance of the studied film, that is, ohmic resistance or ionic charge-transfer resistance (Rct) of the polymer-solution interface by the intercept of the semicircle with the real axis [35, 36]. This behaviour is typical of impedance diagram of polymer film-coated metals in the asymmetric metal/film/electrolyte configuration [37].

Figure 4: Nyquist plots of Pt modified electrode with P3T, recorded in: (a) CH3CN/TBAP, (b) CH2Cl2/TBAP. Plots were recorded in the frequency range from 105 Hz to 10−3 Hz at free potential.

Towards low or middle frequency region, the impedance diagrams show a straight line with slope of 45° which indicates a diffusion-controlled Warburg behavior, attributable to the semiinfinite diffusion of protons at the polymer-electrolyte interface [38].

From the Nyquist plots, the kinetic parameters can be easily deduced. The value of transfer resistance allows us to determine the corresponding capacity C (capacitance of the interface electrode/polymer), using the relationship: 2πfRC = 1 for the frequency where the imaginary part has a maximum value on the half semicircle. The obtained parameters from the impedance plots of P3T are presented in Table 1.

Table 1: Electrical parameters corresponding to P3T in CH3CN/TBAP and in CH2Cl2/TBAP.

As shown from Table 1, the values of Re, Rct, and C are less important in acetonitrile than in dichloromethane medium, indicating that the charge-transfer process of P3T on the Pt electrode is more easier and fast in acetonitrile than in dichloromethane, and the film in CH2Cl2 has a high resistance. These results confirmed what we obtained in cyclic voltametry.

Generally, the electrochemically results obtained from the impedance diagrams of conducting organic polymers are modelled by an equivalent electrical circuit. Many of them have been proposed, in the literature, and in general, for the most part of cases, the equivalent circuit can be assimilated to a circuit of the Randles model, more or less modified according to the experimental conditions. The electrochemical parameters of P3T film are modelled by Randles circuit (Figure 5), which gives the uncompensated electrolyte resistance and serially connected to the capacitance of double layer which is in parallel with the resistance of the charge transfer and Warburg impedance.

Figure 5: Electrical equivalent circuit corresponding to P3T/electrode interface (Randles circuit).

4. Conclusion

Electrochemical characterisation of P3T film was carried out using CV and EIS techniques. CV measurements showed that the electroactivity of polyterthiophene films intensity increases with increase of scan rates and it is more important in CH3CN than in CH2Cl2. However, the reduction peak currents are broader and displaced to more negative potential. EIS revealed that, at high frequencies, charge-transfer process dominates with a semicircle, and at low frequencies, diffusion process dominates with a slope line of 45°. The electrical parameters were found to be more significant in CH3CN.


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