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    Synthesis, properties and application of polyindole/TiO2

    nanocomposites

    This article has been downloaded from IOPscience. Please scroll down to see the full text article.

    2009 J. Phys.: Conf. Ser. 187 012058

    (http://iopscience.iop.org/1742-6596/187/1/012058)

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    Synthesis, properties and application of polyindole/TiO2

    nanocomposites

    Vu Quoc Trung1

    and Duong Ngoc Huyen2

    1Faculty of Chemistry, Hanoi National University of Education,

    136 Xuan Thuy Road, Cau Giay District, Hanoi, Vietnam2Institute of Engineering Physics, Hanoi University of Technology,

    1 Dai Co Viet, Hanoi, Vietnam

    E-mail: [email protected]

    Abstract. Nanocomposites of polyindole (PIn) and TiO2 were prepared by chemicalpolymerization. The morphology of nanocomposite particles was studied by scanning electronmicroscopy and transmission electron microscopy. The chemical structure of conducting polymers in nanocomposites was characterized by FTIR and Raman spectra. The thermalanalysis showed that all conducting polymers in the nanocomposites were stable at more than600oC. The corrosion protection of the nanocomposites was investigated.

    Keywords: Nanocomposite, polyindole, titanium dioxide, corrosion protection.

    1. Introduction

    In recent years, several conducting polymers have received increasing attention as material coatings

    for the protection of common metals against corrosion. In particular, polyaniline and polypyrrole have

    been found to sufficiently reduce the corrosion of steel and other oxidizable metallic materials [13].

    Several reports have been published on polyindole and its derivatives although its close structural

    similarities with polyaniline and polypyrrole [46].

    Polyindole is an electroactive polymer, which can be usually obtained after anodic oxidation of

    indole in various electrolytes; electro-chemical oxidation of indole in LiClO4 containing acetonitrile

    electrolyte medium gives an electrochromic polymer film with good air stability. In its doped state,polyindole has a green colour and an electrical conductivity in the range of 1010 Scm, depending on

    the nature of the counter ion [7, 8]. It is also reported that polyindole films have the advantages of

    fairly good thermal stability, high redox activity and slow degradation rate in comparison with

    polypyrrole and polyaniline [9, 10]. However, there was a lack of reports on the chemical

    electrosynthesis of PIn or PIn composites.

    In this paper, nanocomposites of polyidole and TiO2 were prepared by chemical polymerization.

    The morphology and properties of nanocomposite and were studied by scanning electron microscopy

    (SEM), transmission electron microscopy (TEM), FTIR, Raman spectra and thermal gravimetric

    analysis (TGA). The corrosion protection of the nanocomposites was investigated.

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    Experimental

    1.1. Preparation of nanocomposites

    All nanocomposites were chemically prepared as the procedure described in Ref. [11]. Firstly, a

    dispersion was prepared by mixing (for 30 minutes) of 10.0 g TiO2 (Merk) and 1.0 mL indole

    monomers (Guangzhou Jihuada Chemical, China) in 50.0 ml distilled water. Then 4.5 g FeCl 3 (water-

    free, Fluka Chemie) was added to the oxide particle dispersion during stirring. After 2 hours of

    stirring, the particles were cleaned by distilled water, filtered, extracted for 10 hours and dried at 50oC

    for several days under low pressure.

    1.2. Characterization of nanocomposites

    TGA of prepared samples was measured by Ghimashu-50 H with scan rate of 10oC/min in ambient

    conditions. The X-ray diffraction patterns of TiO2 and TiO2 nanocomposites were measured by

    Simens D-5005. The chemical structure of the nanocomposites was characterized by Fourier transforminfrared spectroscopy (FT-IR) and Raman spectroscopy. FTIR spectra were performed by GBC Cintra

    40-Nicolet Nexus 670 FT-IR. Raman spectra were measured by a Laser Raman spectrophotometer

    (Ramalog 9I, USA). The Van der Pauw method was used to measure the dependencies of dark

    conductivity on reciprocal temperature, as acquired on pressed pellets. The electromagnetic shielding

    features of the nanocomposites were performed by HP8720D Network Analyzer (USA).

    1.3. Investigation of metal corrosion inhibition [12]

    The corrosion inhibition of the PIn/TiO2 nanocomposite was performed by electrochemical methods

    using potentiostatic technique. The electrochemical equipment was AUTOLAP 30 composed from a

    potentiostat in order to make a polarized potential or current. A computer with suitable software

    (GPES) controls the measurement system and analyses the obtained data.

    The solution containing typical eroded ion Cl- (using HCl 3%) was used. The material for corrosioninvestigation was a cylinder (horizontal section: 1 cm), made by the construction steel CT3 (TISCO

    company, produced in Thainguyen, Vietnam) with standard: GOST 001-2001 - TCVN 1656-75 (C:

    0.16 %; Mn: 0.62 %; Si: 0.15 %; P: 0.010 % and S: 0.042 %). Before using, it was polished by rough

    paper 1000, and then cleaned by distilled water and ethanol.

    The sample of the PIn/TiO2 nanocomposite (marked DTC) was prepared as a mixture of 0.1g

    nanocomposite and 1.0 g polyvinyl alcohol (PVA). Then this mixture was covered to be a thin film on

    the surface of the steel. Three other samples were prepared for comparison. The first one was made by

    only 1.0 g PVA (marked D0). The second one was made by a mixture of 0.1 g TiO2 and 1.0 g PVA

    (marked DT). The third one was made by a mixture of 0.1 g PIn and 1.0 g PVA (marked by DP). Then

    these mixtures were covered on the surface of the steel as in the case of the PIn/TiO2 nanocomposite.

    A three-electrode cell was used. A saturated calomen electrode (SCE) was used as reference

    electrode, Pt was the counter electrode and steel bar was the working electrode. All chemicals werepure (PA, China).

    2. Results and discussion

    2.1. Morphology

    Figure 1 shows the SEM image of the PIn/TiO2 nanocomposite particles. The average size of the

    nanocomposite particles was around 60 nm while the average size of TiO2 particles was 50 nm. Figure

    2 shows the TEM image of the PIn/TiO2 nanocomposite particles. The black is TiO2 material and the

    light is the PIn polymer. Generally, SEM and TEM images show that the PIn/TiO 2 nanocomposite

    particles presented with core-shell structure.

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    Figure 1. SEM image of the PIn/TiO2

    nanocomposite particles.

    Figure 2. TEM image of the PIn/TiO2

    nanocomposite particles.

    2.2. Thermal analysis and conductivity of the PIn/TiO2 nanocomposite

    Thermal analysis of the PIn/TiO2 nanocomposite was studied. Below 120oC, the weight reduction is

    originated from water inside samples (1.4%). In the range of 120-330oC, the weight reduction (3.2%)

    is very small, corresponding to the decomposition of redundant oligomers. At higher temperatures

    (300-600oC), the change of weight (10%) is attributed to the decomposition of the oxidized PIn.

    Conductivity of the PIn/TiO2 nanocomposite was performed by two-probe methods with the

    pressed pellet from material powder. It showed that the conductivity of the PIn/TiO 2 nanocomposite is

    1.75 S.cm-1

    . Low conductivity could be explained by the presence of TiO2.

    2.3. FTIR and Raman spectra

    Chemial structure of PIn nanocomposites was characterized by FTIR and Raman scatteringspectroscopy. The FTIR spectrum is of good quality and the infra-red bands are well defined (figure

    3). The spectrum associated with the oxidized PIn are characterized by a very large adsorption band

    located in the spectral domain between 3700 and 3100 cm-1

    , which is characteristic of the OH groups

    belonging to residual water molecules trapped in the polymer matrix as well as water molecules

    absorbed in PIn. The peaks at 3401, 2924, 1593, and 1312 cm-1

    could be attributed to N-H stretching,

    C-H (aromatic) stretching, C=C stretching and C-N stretching (between two idole units), respectively.

    Figure 3. FTIR spectrum of

    PIn/TiO2 nanocomposite.

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    300 600 900 1200 1500 1800

    8000

    16000

    24000

    32000

    40000

    1105

    1330

    1374 1

    460

    1613

    410 5

    10 6

    31

    148

    RamanScattering/a.u

    Wavenumber / cm-1

    Figure 4. Raman spectrum of

    PIn/TiO2 nanocomposite.

    Figure 4 presents Raman spectrum of the PIn/TiO2 nanocomposite measured at 514 nm with 1 mW

    laser power. The peaks at 148, 410, 510, and 631 cm-1

    correspond to the characteristic signals of TiO2.

    The peaks at 1620, 1372, and 1107 cm-1

    were attributed to C=C stretching, C-N stretching and C-H in

    plane deformation.

    2.4. Study of the corrosion inhibition

    The potentiostatic method was applied to study the corrosion inhibition of the eugenol derivatives. The

    curves describing the dependent of the open circuit potential on time (E 0vs. t) are showed in figure 5.

    Value E0 is a parameter to appreciate the corrosion inhibition of samples. It shows that all samples DT,

    DP and DTC had higher E0 than that of D0. It means that these samples could inhibit steel against

    corrosion better than PVA. Among these samples, DTC had highest E0 and, thermodynamically, E0

    presented the best corrosion protection.

    Figure 5. The plots of open circuit

    potential of the test samples vs. time (in

    solution of HCl 3%).

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    Figure 6. Tefel curves of the test

    samples (in solution of HCl 3%).

    Do DT DP DTC

    0.024

    0.032

    0.040

    0.048

    0.056

    icorr

    (mA/cm

    2)

    Sample Figure 7. Corrosion current density ofthe test samples.

    In a 3% solution of HCl, the corrosion inhibition of DTC presented remarkably well by transferring

    positively the Tafel plots (figure 5). Therefore, the corrosion potential was also more positive. From

    Tefel plots and GPES software, the corrosion current density was determined (figure 6). All samples

    containing TiO2, PIn and PIn/TiO2 nanocomposite have lower corrosion current densities, in which

    sample DTC performed the lowest current density.

    Figure 8. Electrochemical

    impedance spectroscopy of the test

    samples (Z is the imaginary part

    and Z is the real part).

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    Figure 8 shows the electrochemical impedance spectroscopy (EIS) of the test samples. The order of

    the impedance is DTC >DP > DT >> D0. By using FRAS software, resistances of the charge transfer

    (Rct) and of the polarization (Rp) were determined (figure 9). It shows both the resistances of thecharge transfer and of the polarization of samples.

    Figure 9. Resistance of charge

    transfer (Rct) and of the

    polarization (Rp).

    Generally, from the results of EIS measurements were in the agreement with open circuit potential

    and corrosion current measurements. These results show that the corrosion inhibition of the PIn/TiO 2

    was the best.

    3. Conclusions

    In this paper, the PIn/TiO2 nanocomposites were prepared by in situ polymerization. SEM and TEM

    imagesshow that the composites are obtained with nanostructure. The chemical structure of PPy in

    nanocomposites was characterized by FTIR and Raman spectra. The thermal analysis TGA showedthat PPy in the nanocomposites was stable at around 600

    oC. The corrosion inhibition of the PIn/TiO2

    nanocomposite was investigated by the polarization and electrochemical impedance methods. It

    showed that the PIn/TiO2 nanocomposite can protect the mild steel against corrosion. It is the

    foundation for producing the environment-friendly paints.

    References

    [1] Tan C K, Blackwood D J 2003 Corros. Sci. 45 545[2] Herrasti P, Ocon P 2001Appl. Surf. Sci.172 276[3] Ahmad N, Mac Diarmid A G 1996 Synth. Met.78 103[4] Sazou D 2002 Synth. Met.130 45[5] Dudukcu M, Yazici B, Erbil M 2004Mat. Chem. Phys. 130 138[6] Ismail A A, Sanad S H, El-Meligi A A 2000J. Mat. Sci. Tech. 16(4)397[7] Billaud D, Maarouf E B, Hannecart E 1994 Polym. Commun. 35 2010[8] Talbi H, Humbert B, Billaud D 1997 Synth. Met. 84 875[9] Billaud D, Maarouf E B, Hannecart E 1995 Synth. Met. 69 571[10] Abthagir P S, Dhanalakshmi K, Saraswathi R 1998 Synth. Met. 93 1[11] Q.-T. Vu, Pavlik M, Hebestreit N, Pfleger J, Rammelt U, Plieth W 2005Electrochim. Acta.51

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    [12] Corrosion Handbook2000 (John Wiley and Sons)

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