Estudios de relajacion dielectrica a altas temperaturas en dioxido de titanio modificado con carbon activado.
Titanium dioxide has been extensively investigated, because of its physicochemical properties that allows it to be a suitable material for a variety of applications (Sergiu et al., 2007; Feng et al, 2008; Yoon et al., 2009). It is a light sensitive semiconductor which absorbs electromagnetic radiation in the region near ultraviolet and it is very stable chemically. By the above features it is the most commonly used photocatalyst and it is currently used as degrader of organic molecules in the water purification process. It is also used as white pigment for its dispersion properties, anticorrosive coating, gas sensor and generally in the ceramics industry (Kubacka et al, 2008; Garcia et al., 2009). This compound have three crystalline phases: rutile (tetragonal structure), anatase (octahedral structure), brookite (orthorhombic structure), which according to the requirement of the electrostatic valence rule, each oxygen atom is shared by three octahedra. For rutile each octahedron has two sides common with other octahedra; in brookite three and for anatase four sides shared by others octahedra. The Ti[O.sub.2] has a band gap of 3.0 eV for rutile phase and 3.2 eV for the anatase phase. These values require ultraviolet radiation (UV) to be activated. Recent research (Barberio et al., 2014. Irie et al., 2003; Ochoa et al., 2009) focus on the possibility of reducing the bandgap size of anatase using doping materials such as nitrogen and carbon, thus taking advantage of the catalytic effect on a significantly larger wave spectrum. For the titanium dioxide doping, carbon has proved to be suitable as external atom, where the incorporation has reduced bandgap of 3.2 eV (pure anatase) to 2.32 eV (carbon doped phase), with which the required wavelength for excitation has been increased to 535 nanometers (Irie et al., 2003; Yoon et al., 2009). Thus, titanium dioxide mixed with carbon has significantly higher effectiveness than pure titanium dioxide. Due to this reported effect caused by the activated carbon on the Ti[O.sub.2] matrix, it is also expected to affect the dielectric properties of the material, because of this, in this paper is studied the effect in the electrical properties of oxide titanium produced by the carbon impurities, for this was realized the electrical characterization of such composites in the form of pressed pellets obtained from commercial powder and different mole fractions of activated carbon using the technique of complex impedance spectroscopy. For it, are analized the Nyquist plots and formalism of the imaginary part of the electrical module in the time domain (Williams & Watts, 1970) for study the dynamic processes of dielectric relaxation of the carriers.
2. Experimental procedure
To prepare the Ti[O.sub.2] mixed with activated carbon samples, it was used Ti[O.sub.2] anatase phase with 99.5% purity (Aldrich), grain size 21 nm ~ and activated carbon powder (Aldrich). It also has been calculated the necessary amount of each for obtain mole fractions of X = 0.09, 0.04, 0.03 and 0.02 using stoichiometric calculation. After this procedure the precursors were mixed by hand macerated in an agate mortar for about three hours, until homogeneity was obtained. Compounds obtained were pressed at room temperature to obtain pill form in a hydraulic press. Infrared spectroscopy of the composites were performed on a spectrometer FTIR mark Shimadzu Prestige 21 with transparent tablets containing the sample and KBr as a binder (90 wt%), the qualitatively determination of the presents functional groups was done using a number of 16 sweeps and a resolution of 4 [cm.sup.-1]. Measures of the complex electrical impedance at high temperatures are performed in a measuring cell adapted to a tubular three-zone furnace Carbolite TZF, this furnace can reach temperatures up to 1473 K. For data acquisition of electrical impedance was used the HIOKY 3532-50 LCR HITESTER equipment in a frequency range between 40Hz and 5MHz and an applied voltage signal of 0.5V. The sample was placed in the measuring cell between two circular shape flat electrodes of gold. Measurements were made from 323K to 723 K at intervals of 50K, in two different atmospheres, nitrogen and helium, with a constant flow and a pressure of 0.2 psi. Finally, adjustments to the experimental curves were obtained by equivalent electrical circuits in the theoretical modeling software Zview2 and by using the decay function of the electric field KWW.
3. Analysis and results
3.1 Characterization for infrared spectroscopy with transformed of Fourier
Figure 1 shows the IR spectra of the samples of Ti[O.sub.2] in different mole fractions of activated carbon. For macerated manually obtained compounds, the spectra shows a band at 3440 [cm.sup.-1], this is associated with the H-OH vibrational mode stress and where the transmittance or infrared absorption carbon increases with decreasing concentration. It was found a band at 2908 [cm.sup.-1] which is due to C-H bonds of aromatic groups, due to the presence of activated carbon, it has been observed that this band decreases drastically by reducing the carbon content. The band at 1630 [cm.sup.-1] corresponds to the water bending mode (Vargas et al., 2011). Looking specifically at the 1000 to 400 [cm.sup.-1] region of the spectrum, a broadband is defined as the activated carbon content increases. The characteristics bands of this region are located at 680 [cm.sup.-1] and can be associated with the vibrational mode of the functional group Ti-O-Ti and the functional group Ti-O (Ochoa et al., 2009). In general, in Figure 1 an increase of intensity with decreasing carbon content is observed, this shows that the formation of the various bounds is stronger at low mole fractions of carbon.
3.2 Complex electrical impedance characterization
Figure 2 shows the Nyquist plot, -Z" vs. Z' for the behavior of the impedance of the composite system Ti[O.sub.2], mixed stoichiometrically with activated carbon mole fractions X = 0.09, 0.03 and Ti[O.sub.2] undoped to a temperature of 313 K at atmospheric pressure and without inert gas. At this temperature the typical impedance spectrum consists of a nonideal semicircle around the frequency range, whose center is displaced under the real axis due to the sample volumetric response and it is not shown the double layer capacitance effect on the interface electrode/electrolyte, characterized by a linear response at low frequency. The non-ideal semicircle observed is modeled using an equivalent circuit (continuous curve) shown on the right side of Figure 2. The circuit consists of a resistor R, a capacitance C and constant phase element (CPE) connected in parallel. Once the resistance of the composite is obtained, it is possible to obtain the values of conductivity-dc of the sample using the [[sigma].sub.0] = d/RA equation, where A and d are the area and thickness of the sample respectively. The values of the setting parameters obtained by the proposed equivalent circuit are presented in Table 1. It is fount that for the obtained composite, the resistance values decrease considerably with increasing content of activated carbon, from 4.40E + 08 [ohm] to Ti[O.sub.2], to 1.69E + 07[ohm] for the highest concentration of carbon X = 0.09. The values found for the capacitor were in the order of picofarads and no appreciable change with the concentration of activated carbon was found. P values of constant phase element parameter reflect a distribution of relaxation times, which is related to phenomena of correlation of carriers in the crystal lattice of the material.
In Figure 3 the Nyquist plot, -Z" (milliohms) vs Z '(milliohms) for Ti[O.sub.2] mixed with activated carbon for a molar ratio of X = 0.09, obtained under nitrogen at a temperature range between 323K, 723K and a pressure 0.2 psi. The different discrete symbols correspond to the experimental data representing the dielectric response of the composite, while the continuous curve represents the adjustment data obtained by the same equivalent circuit used in the above analysis. The electrical response as a function of temperature has a well-defined region in the entire frequency range, which is shaped like a not ideal semicircle due to the predominance of the dielectric response of the material over the conductor behavior. The values obtained for the different adjustment parameters are presented in Table 2. It is found in the upper diagram of Figure 3 that the volume resistance value R1 increases progressively with increasing temperature from 323-523 K. Moreover it shows that the resistance decreases as the temperature increases from 523K, which is a typical behavior of semiconductor materials. Moreover, the volume Capacitance of the sample is mostly of the order of picofarads and varies very little with increasing temperature. It is found that the value of parameter P ofthe constant phase element, decreases significantly from 323-523 K, showing that the system becomes more capacitive and the relaxation of induced dipoles in the material is highly correlated with increasing temperature, whereas for temperatures above 523 K, it retakes values close to one, showing that the relaxation of oriented dipoles is very close to the Debye type behavior.
In the Figure 4 it is shown the Nyquist plot, -Z" (milliohms) vs Z '(milliohms), for Ti[O.sub.2] mixed with activated carbon for the same molar ratio X = 0.09, but now the data is obtained in helium atmosphere in a temperature range of 323K to 473K and a pressure-0.2 psi. Experimental data were modeled with the same equivalent circuit (continuous curve) and is found that the resistance increases with increasing temperature, opposite to the observed behavior under nitrogen. Capacitance values (Table 2) of the sample are in the order of picofarads and does not change appreciably with temperature increases, as observed under nitrogen. Moreover, the value of the P parameter of the constant phase element is very close to one, showing that the orientation of the dipoles induced by applying external electric field is not highly correlated and approaches to a Debye behavior.
The dynamics of the induced dipole orientation when applying the external electric field is analyzed with the electric modulus formalism and the following relationship,
Where, [M.sup.*] ([omega]) is the electrical modulus and [M.sub.[infinity]] represents the value of its real part at high frequencies. In the equation is used the Kohlrausch-WilliamsWatts (KWW) function (Williams & Watts,1970).
[mathematical expression not reproducible] (2)
Where 0 <[beta] <1 is an exponent indicating the Debye relaxation deviation ([beta] = 1) and t represents a characteristic relaxation time.
The imaginary modulus M"([omega]) for the Ti[O.sub.2] plus activated carbon composite with x=0.09 concentration, obtained in a first heating under a nitrogen atmosphere and applying a potential of 0.5 V, shown in Figure 5. The points correspond to the experimental data and solid line corresponds to the adjustment obtained using equation 1. The imaginary module has a maximum whose value decreases and the peak position with the frequency shifts to the low frequency region at increases of the temperature, evidencing the existence of a relaxation process associated with the orientation of dipoles of the composite system, which is thermally deactivated. The relaxation frequency [omega]p corresponds to Mmax, given the more probable relaxation time Tp by the condition [[tau].sub.p] [[omega].sub.p] = 1 (Macdonald et al., 2005). The asymmetric and broad shape of the imaginary part of the electrical module is described by the exponent p of the exponential KWW function. The p exponent values found in the fit, change depending on the temperature and range from a value of [beta] = 0.68 at 323 K, to [beta] = 0.47 to 523 K. These values of p clearly indicate that the relaxation process of induced dipoles goes away of a Debye type behavior for an increasing temperature. The ease or difficulty of a molecule to be reoriented in a solid depends on its shape and its interactions with their environment, according with the applied temperature and the inclusion of dopant in the material the relaxation time will change. Usually, in the measures at a range of frequencies higher than the characteristic relaxation frequency, the contribution to the electrical modulus is not observed. Physically, it happens that the applied frequency for measurement is too high and the dipoles cannot follow the oscillations of the applied electric field, therefore these dipoles do not participate in the polarization of the material (Jonscher, 1999). The fact that the peak of the module moves to lower frequencies and is much wider with increasing temperature, responds to the stabilization of the amorphous walls of Ti[O.sub.2] with consequent delay of the crystallization temperature caused by the presence of carbon. Furthermore, for high mole fractions of carbon, a presumably crystallization has occurred due to the high dispersion of the carbon particles in the matrix of Ti[O.sub.2], being strongly delayed the temperature of transformation. Moreover for an nitrogen atmosphere is produced an anionic doping where an anion (A) of Nitrogen enters the Ti[O.sub.2] network to substitute an oxygen atom and form Ti[O.sub.2-x] [A.sub.x] (Sauthier et al., 2012).
In Figure 6 is shown the M ([omega]) imaginary part of the modulus for a system formed by Ti[O.sub.2] with a molar fraction of activated carbon X = 0.09, obtained by heating the sample in a helium atmosphere and applying a potential of 0.5 V, as shown in figure 5 the points correspond to the experimental data and the solid line corresponds to the setting obtained using equation 1. When the sample is subjected to a helium atmosphere, the modulus imaginary part has a maximum whose value remains approximately constant and contrary to what is presented in a nitrogen atmosphere, the peak position in function of the frequency shifts to the high frequency region with increases of the temperature, giving evidence of the existence of a relaxation process associated with the orientation of dipoles of the composite system, which it is thermally activated. The values of P exponent found in the fit increases progressively with increasing temperature from a value of [beta] = 0.45 at 323 K, to [beta] = 0.64 at 523 K. The values of P exponent obtained for a sample in the presence of an atmosphere of helium are completely different from those obtained for a sample under a nitrogen atmosphere, indicating the great influence of the kind of atmosphere in the processes of dipole orientation induced in the composite. The values of the setting parameters are reported in Table 5, the lines in various boxes, means that it is not possible to obtain the value because the experimental curve of the imaginary part of the electrical modulus does not have a maximum well defined or it cannot be solve in the frequency range of the impedance meter. Similar behavior is studied for other composites, with different mole fractions of activated carbon.
The addition of activated carbon in the matrix of the obtained titanium oxides does not produce significant changes in the vibrational modes of Ti[O.sub.2]. The values of the proposed equivalent circuit parameters show that the sample under nitrogen atmosphere presents higher resistance values with the increase of the temperature, opposite to the process that presents the sample under helium atmosphere, which means that the Ti[O.sub.2] mixed with activated carbon, can be used as gas sensor. Meanwhile the value of the P exponent of KWW model shows a relaxation process of induced dipole which is disfavored with increasing temperature when the sample is subjected to a nitrogen atmosphere. The results of the dielectric response of the studied composites, suggest that nitrogen produces a anionic doping, where an anion (A) of Nitrogen enters in the network of Ti[O.sub.2] to substitute an oxygen and form Ti[O.sub.2-x] [A.sub.x].
Barberio, M., Barone, P., Imbrogno, A., Ruffolo, S.A., La Russa, M., Arcuri, N. & Xu, F. (2014). Study of Band Gap of Carbon Nanotube-Titanium Dioxide Heterostructures. Journal of Chemistry and Chemical Engineering 8 (1), 36-41.
Feng, X., Shankar, K., Varghese, O.K., Paulose, M., Latempa, T.J. & Grimes, C.A. (2008). Vertically
Aligned Single Crystal Ti[O.sub.2] Nanowire Arrays Grown Directly on Transparent Conducting Oxide Coated Glass: Synthesis Details and Applications. Nano Lett 8 (11), 3781-3786.
Garcia, H., Llabres, F., Perez, E. D., Artigas, R., Raya, F., Sierra, F. & Campos, J. L. R. (2009). Porcelanico Bionictiler: reduccion selectiva de NOx ambiental con productos ceramicos esmaltados aditivados con una composicion conteniendo dioxido de titanio y potenciadores. Boletin de la Sociedad Espanola de Ceramica y Vidrio 48 (2), 91-94.
Irie, H., Watanabe, Y. & Hashimoto, K. (2003). Carbon-doped Anatase Ti[O.sub.2] Powders as a Visiblelight Sensitive Photocatalyst. Chemistry Letters 32 (8), 772-773.
Jonscher, A.K. (1999). Dielectric relaxation in solids.
Journal of Physics D: Applied Physics 32 (14), R57.
Kubacka, A., Ferrer, M., Fernandez-Garcia, M., Cerrada, M. L., Serrano, C., Sanchez-Chaves, M. & Fernandez-Martin, F. (2008). Sistemas biocidas basados en Ti[O.sub.2] con aplicacion en la industria alimentaria. Eurocarne 18 (164), 61-68.
Macdonald, J.R. & Johnson, W.B. (2005). Fundamentals of impedance spectroscopy. Impedance Spectroscopy: Theory, Experiment, and Applications. Second Edition ed. New Jersey: John Wiley & Sons, Inc.
Ochoa, Y., Ortegon, Y., Vargas, M. & Paez, JR. (2009). Sintesis Ti[O.sub.2], fase Anatasa, por el metodo Pechini. Suplemento de la Revista Latinoamericana de Metalurgia y Materiales S 1 (3), 931-937.
Ohno, T., Mitsui, T. & Matsumura, M. (2004). Photocatalytic Activity of S-doped Ti[O.sub.2] Photocatalyst under Visible Light. Chemistry Letters 256 (1), 364-365.
Sauthier, G. (2012). Preparacion y caracterizacion de capas delgadas y estructuras de oxido de titanio para aplicaciones fotocataliticas activadas mediante radiacion UVo visible. Doctoral Thesis, Instituto de Ciencia de Materiales de Barcelona, Universidad Autonoma de Barcelona, Barcelona, Espana.
Sergiu, P.A., Andrei, G., Jan, M.M., Robert, H. & Patrik, S. (2007). Self-Organized, FreeStanding Ti[O.sub.2] Nanotube Membrane for Flow- through Photocatalytic Applications. Nano Lett 7 (5), 12861289.
Vargas-Urbano, M.A., Ochoa-Munoz, Y. H., Ortegon-Fernandez, Y., Mosquera, P., RodriguezPaez, J.E. & Camargo-Amado, R.J. (2011).
Nanoparticulas de Ti[O.sub.2], fase anatasa, sintetizadas por metodos quimicos. Ingenieria Y Desarrollo 29 (2), 186-201.
Williams, G. & Watts, D.C. (1970). Non-symmetrical dielectric relaxation behaviour arising from a simple empirical decay function. Transactions of the Faraday Society 66, 80-85.
Yoon, S., Bok, H.K., Lee, C., Park, M. & Oh, S.M. (2009). Preparation of Nanotube Ti[O.sub.2] Carbon Composite and Its Anode Performance in LithiumIon Batteries. Electrochemical and SolidState Letters 12 (2), 28-32.
Karen A. Castaneda * ([seccion]), Ingrith P. Cuellar *, Jose H. Castillo *
* Facultad de Ciencias Basicas y Tecnologias, Programa de Fisica, Grupo de Fisica de Materiales Inorganicos y Organicos (FMIO), Universidad del Quindio. Armenia, Quindio.
([seccion]) firstname.lastname@example.org, email@example.com, firstname.lastname@example.org
(Recibido: Noviembre 25 de 2015-Aceptado: Febrero 19 de 2016)
Caption: Figure 1. FTIR spectra of the samples oof Ti[O.sub.2] in different mole fractions oof activated carbon.
Caption: Figure 2. Nyquist plot for the composite formed for Ti[O.sub.2] mixed stoichiometrically with activated carbon mole fractions, obtained at a temperature oof 313 K and a potential oof 0.5 V
Caption: Figure 3. Nyquist plot for a mole fraction of X=0.09 under nitrogen, in a temperature range of 323K-623K and potential 0.5V.
Caption: Figure 4. Plot Nyquist for the composite formed forTi[O.sub.2] mixed stoichiometrically with activated carbon with mole fraction of X=0.09 under helium in a temperature range of 323K-473 K.
Caption: Figure 5. Imaginary part of the electrical module in function of frequency for a molar fraction X=0.09 under nitrogen and temperatures 323K to 573K.
Caption: Figure 6. Imaginary part of the electrical module in function of frequency for a molar fraction X=0.09 under helium and temperatures 323K to 723K..
Table 1. Parameter values of the equivalent circuit for the TiO2 mixed stoichiometrically with activated carbon mole fractions, obtained at a temperature of 313 K. Concentration R1(M[OMEGA]) CP1-T CP1-P C1 (PF) [+ or -]0.02 [+ or -] 0.02 X=0,09 1.69E+07 6.94E-11 0.73 4.72E-12 X=0,03 2.25E+07 2.73E-10 0.55 3.87E-12 Ti[O.sub.2] 4.40E+08 7.70E-11 0.64 9.41E-12 Table 2. Parameter values ofthe equivalent circuit for the Ti[O.sub.2] mixed stoichiometrically with activated carbon to a mole fraction X=0.09 under nitrogen. T (K) R1(M[OMEGA]) CP1-T CP1-P C1 (PF) [+ or -] 0.02 [+ or -] 0.02 323 0.50 2.20E-09 0.55 13.1 373 3.00 3.15E-06 0.49 50.00 423 12.41 3.43E-06 0.42 32.11 473 29.53 1.79E-06 0.47 32.11 523 54.68 1.90E-06 0.47 32.11 573 19.59 7.93E-07 0.61 31.08 623 13.78 1.88E-07 0.74 12.85 673 13.78 1.88E-07 0.74 12.85 Table 3. Parameter values of the equivalent circuit for the composite system formed for Ti[O.sub.2] mixed stoichiometrically with activated carbon with mole fraction X=0.09 under helium. T(K) R1(M[OMEGA]) CP1-T CP1-P C1(PF) [+ or -] 0.02 [+ or -]0.02 323 2.51 4,12 E-9 0.50 11.40 373 0.58 1,51E-09 0.77 9.51 423 0.46 3,23E-10 0.77 2.14 473 0.34 2,35E-09 0.77 8.00 Table 4. Adjustment parameters obtained by the model KWW for the Ti[O.sub.2] mixed stoichiometrically with activated carbon to a mole fraction X=0.09 under nitrogen. T(K) B [+ or -] Log Wn(Hz) M"max 0.01 [+ or -]0.01 323 0.68 5.05 11.05 373 0.67 4.28 10.42 423 0.62 3.80 10.62 473 0.53 3.55 10.62 523 0.53 3.57 9.62 573 0.47 3.75 10.02 Table 5. Adjustment parameters obtained by the model KWW for the composite system Ti[O.sub.2] mixed stoichiometrically with activated carbon mole fraction X=0.09 under helium. T(K) p [+ or -] Log Wn(Hz) M"max 0.01 [+ or -] 0.01 323 0.45 5.25 34.60 373 0.45 5.70 37.00 423 0.45 5.81 37.50 473 0.45 6.00 40.00 523 0.45 7.60 36.80 573 0.63 8.00 78.60 623 0.64 8.30 13.60 673 0.64 8.70 9.60 723 0.64 8.80 7.60
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|Title Annotation:||INGENIERIA DE MATERIALES|
|Author:||Castaneda, Karen A.; Cuellar, Ingrith P.; Castillo, Jose H.|
|Publication:||Ingenieria y Competividad|
|Date:||Jun 1, 2017|
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