# The Use of Le Bail Method to Analyze the Semicrystalline Pattern of a Nanocomposite Based on Polyaniline Emeraldine-Salt Form andα-Al2O3

Authors: Edgar A. Sanches; Adriano de S. Carolino; Amanda L. dos Santos; Edson G. R. Fernandes; Daniela M. Trichês; Yvonne P. Mascarenhas
Journal: Advances in Materials Science and Engineering
 (2015)

---

## Abstract

Ceramic nanocomposites constituted by a matrix ofα-Al2O3 microparticles reinforced by polyaniline emeraldine-salt form (PANI-ES) nanoparticles were prepared byin situ polymerization and characterized structural and morphologically. Peaks related to both materials were observed through XRD technique: PANI-ES presented peaks at 2
θ = 8.9, 14.9, 20.8, 25.3, 27.1, and 30.0° and in α-Al2O3 phase peaks were found at 2
θ = 25.6, 35.2, 37.9, 43.5, 52.6, 57.6, and 68.1°. Nanocomposite crystallinity percentage was estimated around 70%. SEM showed a polymerization of PANI-ES over alumina plates. By Le Bail method it was observed that PANI-ES and α-Al2O3 have crystallite average size around, respectively, 41 and 250 Å. By FTIR analysis characteristic absorption bands of both materials were identified. Additional bands indicating new chemical bonds were not observed, suggesting that nanocomposite was formed by physical deposition. Nanocomposite DC electrical conductivity was found around 0.24 S/cm (against 1.84
×
10
-
4 S/cm for pure PANI-ES), showing an increase of about 1,300 times compared to the pure PANI-ES at room temperature. Thus, this paper showed that both materials have kept its original structural characteristics and exhibited high electrical conductivity when combined in nanocomposite form.


---

## Body

## 1. Introduction

Interest in nanocomposites (NCs) has grown considerably because these materials tend to exhibit better properties when compared to conventional composites [1–4]. The improvement in their properties occurs due to the fact that the interactions at the interface between matrix/reinforcement tend to increase in nanoscale [5–7]. NCs constituted by polyaniline (PANI) or its derivatives and aluminum oxide have been prepared by several methods, resulting in a range of applications [8–16].Intrinsically conducting polymers (ICPs) have been widely studied due to its great potential in technological applications, representing a class of materials with mechanical, electrical, and optical properties similar to metals and inorganic semiconductors [17–21]. Among ICPs, polyaniline emeraldine-salt form (PANI-ES) has a prominent position due to the low cost of monomer, ease of synthesis, and doping and chemical stability [22–26]. Aluminum oxide (α-Al2O3) is one of the most important advanced ceramic materials due to its good corrosion resistance, hardness, good mechanical properties, and adsorption capacity, which favor its use in several technological applications [27–31].Despite the importance of PANI in the ICPs class, there are some limitations that hinder its use in industrial scale, such as low solubility in organic solvents, low mechanical flexibility, and processability [32, 33]. A widely used mechanism for improving its solubility and processability is the introduction of polar functional and long flexible alkyl groups mainly bonded to the main chain [34]. Furthermore, PANI is one of the most promising industrial alternatives to obtain nanocomposites or blends. Then, one can combine the electrical properties of PANI with mechanical properties of the insulating matrix, such as alumina [35].Nanocomposite constituted byα-Al2O3 microparticles reinforced by PANI-ES nanoparticles was prepared byin situ polymerization. Fourier-transform infrared spectroscopy (FTIR) was used for bonds of structural information; XRD was used for the determination of cell parameters and crystallinity percentage estimative; Le Bail method was performed to refine cell parameters and to obtain crystallite size and shape; SEM was carried out for the determination of solid nanocomposite morphology. These results were correlated with electrical properties. The crystal structure investigation of semicrystalline materials is an important research topic in many areas and remains in full development. Understanding the structure of semicrystalline nanocomposites constituted by polymer/ceramic materials is essential to the development of new technological applications.


## 2. Experimental

### 2.1. Nanocomposite Synthesis

PANI-ES/α-Al2O3 synthesis was performed based on Zhang (2006) [8] and Sanches et al. (2013) [25], with some modifications. Aniline (ANI) monomer was purchased from Sigma-Aldrich and further distilled. α-Al2O3 was obtained from Sapra, SA; São Carlos, SP, in December 2013. Two solutions were prepared. In Solution I, 20 mL of distilled aniline (ANI) was dissolved in 500 mL of hydrochloric acid (HCl) 1.0 M, added to 167 g of α-Al2O3 powder under stirring. In Solution II, 11.5 g of ammonium persulfate (APS) was added to 200 mL of hydrochloric acid (HCl) 1.0 M. Then, Solution II was rapidly added to Solution I allowing the polymerization. System remained under stirring for 3 h. Then, the dispersion of green color with α-Al2O3 particles was vacuum filtered and washed with acetone.


### 2.2. Fourier-Transformed Infrared Spectroscopy (FTIR)

Infrared spectra were measured inNanomed Inovação em Nanotecnologia in a spectrophotometer Bomem-MB Series-Hartmann and Braun in the range of 400–2000 cm−1. Samples were prepared in KBr pellet with mass ratio of 1 : 100.


### 2.3. X-Ray Diffraction and Crystallinity Percentage

XRD data were obtained at the Laboratory of X-ray Crystallography of IFSC/USP, São Carlos, SP, using a Rigaku Rotaflex diffractometer equipped with graphite monochromator and rotating anode tube, operating with Cu Kα, 50 kV, and 100 mA. Powder diffraction patterns were obtained in step scanning mode, 2
θ = 5–55°, step of 0.02°, and 3 s/step. Using routine software, crystallinity percentage was estimated using the diffractogram pattern and separating and then measuring the integrated intensities from the crystalline and noncrystalline phases. The integration was carried out over the whole range 2
θ = 5° to 55°, where θ is the Bragg angle. The estimated crystallinity (E.C.), given as a percentage, was obtained by E.C.
=
100
A
c
/
(
A
a
+
A
c
), where A
c and A
a are, respectively, the crystalline and noncrystalline integrated intensities [36].


### 2.4. Le Bail Method

The use of Le Bail whole powder pattern decomposition method [37] to obtain structural information from semicrystalline patterns is not very common due to the large overlapped peaks on diffractograms. Nevertheless it has been used to characterize polyurethane, polyaniline, and substituted polyanilines [25, 38, 39]. Le Bail method was performed using the software package FullProf [40]. All parameters were refined by the least-squares method [41]. The pseudo-Voigt function modified by Thompson-Cox-Hastings was used as peak profile function [42]. Instrumental resolution function parameters were obtained from a lanthanum hexaborate standard, LaB6. Aniline tetramer single crystal parameters obtained by Evain et al. [43] were used as initial parameters for PANI phase (a = 5.7328 Å, b = 8.8866 Å, c = 22.6889 Å, α = 82.7481°, β = 84.5281°, and γ = 88.4739°). Aluminum oxide structural parameters obtained by Lutterotti and Scardi [44] were used as initial parameters for alumina phase (a = 4.756 Å, b = 4.756 Å, c = 12.9636 Å, α = 90.0°, β = 90.0°, and γ = 120.0°). Anisotropic crystallite size was determined using spherical harmonics (SHP) [45–47].


### 2.5. SEM Analysis and DC Conductivity Measurements

SEM experiments were performed in equipment Supra 35, Carl Zeiss. Powder samples were deposited on a carbon tape and the surface morphology was obtained at room temperature. For DC conductivity measurements, samples processed into pellets were coated with silver ink on both sides in which electrical connections were made. Measurements were performed at room temperature (300 K) using a Keithley Model 2612 A from 500 mV to 2 V.


## 2.1. Nanocomposite Synthesis

PANI-ES/α-Al2O3 synthesis was performed based on Zhang (2006) [8] and Sanches et al. (2013) [25], with some modifications. Aniline (ANI) monomer was purchased from Sigma-Aldrich and further distilled. α-Al2O3 was obtained from Sapra, SA; São Carlos, SP, in December 2013. Two solutions were prepared. In Solution I, 20 mL of distilled aniline (ANI) was dissolved in 500 mL of hydrochloric acid (HCl) 1.0 M, added to 167 g of α-Al2O3 powder under stirring. In Solution II, 11.5 g of ammonium persulfate (APS) was added to 200 mL of hydrochloric acid (HCl) 1.0 M. Then, Solution II was rapidly added to Solution I allowing the polymerization. System remained under stirring for 3 h. Then, the dispersion of green color with α-Al2O3 particles was vacuum filtered and washed with acetone.


## 2.2. Fourier-Transformed Infrared Spectroscopy (FTIR)

Infrared spectra were measured inNanomed Inovação em Nanotecnologia in a spectrophotometer Bomem-MB Series-Hartmann and Braun in the range of 400–2000 cm−1. Samples were prepared in KBr pellet with mass ratio of 1 : 100.


## 2.3. X-Ray Diffraction and Crystallinity Percentage

XRD data were obtained at the Laboratory of X-ray Crystallography of IFSC/USP, São Carlos, SP, using a Rigaku Rotaflex diffractometer equipped with graphite monochromator and rotating anode tube, operating with Cu Kα, 50 kV, and 100 mA. Powder diffraction patterns were obtained in step scanning mode, 2
θ = 5–55°, step of 0.02°, and 3 s/step. Using routine software, crystallinity percentage was estimated using the diffractogram pattern and separating and then measuring the integrated intensities from the crystalline and noncrystalline phases. The integration was carried out over the whole range 2
θ = 5° to 55°, where θ is the Bragg angle. The estimated crystallinity (E.C.), given as a percentage, was obtained by E.C.
=
100
A
c
/
(
A
a
+
A
c
), where A
c and A
a are, respectively, the crystalline and noncrystalline integrated intensities [36].


## 2.4. Le Bail Method

The use of Le Bail whole powder pattern decomposition method [37] to obtain structural information from semicrystalline patterns is not very common due to the large overlapped peaks on diffractograms. Nevertheless it has been used to characterize polyurethane, polyaniline, and substituted polyanilines [25, 38, 39]. Le Bail method was performed using the software package FullProf [40]. All parameters were refined by the least-squares method [41]. The pseudo-Voigt function modified by Thompson-Cox-Hastings was used as peak profile function [42]. Instrumental resolution function parameters were obtained from a lanthanum hexaborate standard, LaB6. Aniline tetramer single crystal parameters obtained by Evain et al. [43] were used as initial parameters for PANI phase (a = 5.7328 Å, b = 8.8866 Å, c = 22.6889 Å, α = 82.7481°, β = 84.5281°, and γ = 88.4739°). Aluminum oxide structural parameters obtained by Lutterotti and Scardi [44] were used as initial parameters for alumina phase (a = 4.756 Å, b = 4.756 Å, c = 12.9636 Å, α = 90.0°, β = 90.0°, and γ = 120.0°). Anisotropic crystallite size was determined using spherical harmonics (SHP) [45–47].


## 2.5. SEM Analysis and DC Conductivity Measurements

SEM experiments were performed in equipment Supra 35, Carl Zeiss. Powder samples were deposited on a carbon tape and the surface morphology was obtained at room temperature. For DC conductivity measurements, samples processed into pellets were coated with silver ink on both sides in which electrical connections were made. Measurements were performed at room temperature (300 K) using a Keithley Model 2612 A from 500 mV to 2 V.


## 3. Results and Discussion

### 3.1. FTIR Analysis

Figure1 shows the FTIR spectra of the nanocomposite (PANI-ES/α-Al2O3), PANI-ES, and α-Al2O3. For PANI-ES spectrum, bands were found between 1556 and 1457 cm−1 (band 1), which were related to C=C double bonds; bands between 1300 and 1234 cm−1 (band 2) are due to the C–N stretching; a band located at 1132 cm−1 (band 3) is attributed to vibration of C–H bond and 794 cm−1 (band 4) to the out-of-plane angular vibration of C–H aromatics. Regarding the α-Al2O3 phase, bands between 649 and 457 cm−1 correspond to the condensed AlO6 octahedra which compose the building blocks in α-Al2O3 structure [48]. Thus, in the FTIR nanocomposite spectrum bands related to both materials were observed. No additional bands related to new chemical bonds were found, suggesting that the nanocomposite was formed by physical deposition.Figure 1
FTIR of PANI-ES,α-Al2O3, and nanocomposite.


### 3.2. X-Ray Diffraction and Crystallinity Percentage

By XRD technique the diffraction pattern of the nanocomposite PANI-EB/α-Al2O3 was obtained. Peaks related to both materials were observed in diffractogram. With respect to PANI-ES, peaks were found at 2
θ = 8.9, 14.9, 20.8, 25.3, 27.1, and 30.0° [25] and for α-Al2O3 phase peaks were present at 2
θ = 25.6, 35.2, 37.9, 43.5, and 52.6° [44]. Figure 2 shows the nanocomposite XRD pattern. Crystallinity percentage was estimated from the whole nanocomposite XRD pattern. Figure 3 shows the superposition of the diffraction pattern of nanocomposite (PANI-ES/α-Al2O3) (black), the supposed profile related to the noncrystalline phase (red), and the corresponding profile of the supposed crystalline phase (dark blue). Nanocomposite crystallinity percentage was estimated around 70%.Figure 2
Nanocomposite X-ray diffraction pattern.Figure 3
Decomposition of the POEA-ES diffraction peaks.


### 3.3. SEM Analysis and DC Conductivity Measurements

Scanning electron microscopy (SEM) technique revealed that the ceramic material has particles with a range of micrometric sizes with plates-like morphology. For PANI-ES nanosized particles with morphologies similar to interconnected nanospheres were observed, which form the polymer nanofibers. Figures4, 5(a), and 5(b) show, respectively, the morphologies of alumina and PANI-ES. In the nanocomposite it was observed that polymerization of PANI-ES occurred on the α-Al2O3 plates by physical deposition (as suggested by FTIR analysis), being possible to observe in Figures 6(a)–6(c) the morphology of both materials combined in nanocomposite form.Figure 4
SEM image ofα-Al2O3.SEM image of PANI-ES with increase of (a) 31,000 and (b) 100,000 times.
(a)
(b)SEM images of PANI-ES/α-Al2O3 nanocomposite.
(a)
(b)
(c)An increasing about 1,300 times in nanocomposite DC electrical conductivity (0.24 S/cm) was verified when compared to the pure sample of PANI-ES [25]. This is surprising since alumina is an electrical insulator with DC electrical conductivity about 10−14 S/cm. The pure PANI-ES conductivity was found around 1.84
×
10
-
4 S/cm for Sanches et al. [25], as expected.We suggest that the most compact PANI-ES interface between theα-Al2O3 plates contributed significantly to increasing the nanocomposite DC electrical conductivity. The conductive polymer over the α-Al2O3 plates surface (percolation threshold) might promoted easier paths for the charge carriers. Zhang [8] obtained a conductive value of 0.17 S/cm for core-shell structured alumina-polyaniline particles. Michálek et al. [49] studied the electrical conductivity in alumina/multiwall carbon nanotubes (MWCNT) that obtained an increase from 10−14 S/cm (pure alumina) to 2.7
·
10
-
3 S/cm for composites. However, the DC electrical conductivity can decrease in the case of a better interaction between the composite components: Teoh et al. [50] synthesized nanofibers composite by oxidative polymerization of aniline with alumina nanofibers and the DC electrical conductivity decreased with increasing alumina nanofibers from 0.18 S/cm to 10−3 S/cm for alumina loading from 0% to 20%.


### 3.4. Le Bail Method Analysis

A process using iteratively the Rietveld decomposition formula for whole powder pattern decomposition (WPPD) purposes was first applied in 1988 [37] and called much later the “Le Bail method” or “Le Bail fit,” or “pattern matching” as well as “profile matching” in the FullProf Rietveld program [40]. In the original computer program first applying that method, arbitrarily all equal S
k
(
calc
)
2 values are first used, instead of using structure factors calculated from the atomic coordinates, resulting in “I
k
(
obs
)” which are then reinjected as new S
k
(
calc
)
2 values at the next iteration, while the usual profile and cell parameters (but not the scale) are refined by least squares. Equipartition of exactly overlapping reflections comes from the strictly equal result for Bragg peaks at the same angles which would have starting equal calculated intensities. Not starting from a set of all equal S
k
(
calc
)
2 values would produce I
k
(
obs
) values keeping the same original ratio for the exactly overlapping reflections. It is understandable that such an iterative process requires as good starting cell and profile parameters as the Rietveld method itself [51].To perform Le Bail method the crystal symmetry and unit cell for PANI and aluminum oxide obtained, respectively, by Evain et al. [43] and Lutterotti and Scardi [44] were used as input data. The refinement steps were followed by refining the peak width, refinement of a
,
b
,and  c and a
,
b
,
c
,
α
,
β, and γ. This sequence was addressed for both phases. Figure 7 shows the final refinement, with the observed (I
obs, black) and the calculated (I
calc, red) diffractograms, as well as the residual line (I
obs
-
I
calc, blue). Table 1 shows the refined parameters.Table 1
Comparison between the values found by Evain et al. (2002) [43] and Lutterotti and Scardi (1990) [44] with those found by PANI-ES and α-Al2O3, respectively, through Le Bail method.
Refined parameters
Evain et al., (2002) [43]
PANI-ES
Lutterotti and Scardi (1990) [44]
α-Al2O3
a (Å)
5.7328(1)
5.754363
4.7540(5)
4.756846
b (Å)
8.8866(2)
8.855334
4.7540(5)
4.756846
c (Å)
22.6889(6)
22.961094
12.9820(6)
12.966290
α (°)
82.7481(8)
84.222496
90
90
β (°)
84.5281(8)
84.180656
90
90
γ (°)
88.4739(11)
88.148727
120
120
V (Å3)
1141.3(4)
1160
254.1
254.0
Global average size (anisotr.) (Å)
—
41(10)
—
250(40)
Crystallite apparent size100 (Å)
—
46
—
140
Crystallite apparent  size010 (Å)
—
30
—
140
Crystallite apparent  size001 (Å)
—
35
—
90
R
wp (%)
9.3
R
p (%)
5.1
χ
2
6.6Figure 7
Le Bail method applied to nanocomposite.The refined parameters values ​​were compared with those obtained in literature [43, 44]. It is important to stress that the standard deviation appearing in the global average apparent size is calculated using the reciprocal lattice directions so it is a measure of the degree of anisotropy, not of the estimated error. The crystallite size projections for ES-PANI are showed in Figure 8(a). The crystallite shape can be described as a prolate ellipsoidal shape with its longer axis roughly parallel to [
110
] [25]. There was an average crystallite size around 41 Å with standard deviation (anisotropy) of 10 Å. There are a smaller apparent size of 30 and 35 Å in the [
010
] and [
001
] directions, respectively, and others almost equivalent (46 Å) along [
100
]. The crystallite size projections for α-Al2O3 are showed in Figure 8(b). There was an average crystallite size around 250 Å with standard deviation (anisotropy) of 40 Å. There is a largest apparent size of 140 Å in the [
100
] and [
010
] directions, and other smaller (90 Å) along [
001
]. Through Le Bail method it was verified that nanocomposite phases have kept its lattice parameters and provide structural information about crystallite size and shape.Crystallite shapes for (a) PANI-ES and (b)α-Al2O3.
(a)
(b)


## 3.1. FTIR Analysis

Figure1 shows the FTIR spectra of the nanocomposite (PANI-ES/α-Al2O3), PANI-ES, and α-Al2O3. For PANI-ES spectrum, bands were found between 1556 and 1457 cm−1 (band 1), which were related to C=C double bonds; bands between 1300 and 1234 cm−1 (band 2) are due to the C–N stretching; a band located at 1132 cm−1 (band 3) is attributed to vibration of C–H bond and 794 cm−1 (band 4) to the out-of-plane angular vibration of C–H aromatics. Regarding the α-Al2O3 phase, bands between 649 and 457 cm−1 correspond to the condensed AlO6 octahedra which compose the building blocks in α-Al2O3 structure [48]. Thus, in the FTIR nanocomposite spectrum bands related to both materials were observed. No additional bands related to new chemical bonds were found, suggesting that the nanocomposite was formed by physical deposition.Figure 1
FTIR of PANI-ES,α-Al2O3, and nanocomposite.


## 3.2. X-Ray Diffraction and Crystallinity Percentage

By XRD technique the diffraction pattern of the nanocomposite PANI-EB/α-Al2O3 was obtained. Peaks related to both materials were observed in diffractogram. With respect to PANI-ES, peaks were found at 2
θ = 8.9, 14.9, 20.8, 25.3, 27.1, and 30.0° [25] and for α-Al2O3 phase peaks were present at 2
θ = 25.6, 35.2, 37.9, 43.5, and 52.6° [44]. Figure 2 shows the nanocomposite XRD pattern. Crystallinity percentage was estimated from the whole nanocomposite XRD pattern. Figure 3 shows the superposition of the diffraction pattern of nanocomposite (PANI-ES/α-Al2O3) (black), the supposed profile related to the noncrystalline phase (red), and the corresponding profile of the supposed crystalline phase (dark blue). Nanocomposite crystallinity percentage was estimated around 70%.Figure 2
Nanocomposite X-ray diffraction pattern.Figure 3
Decomposition of the POEA-ES diffraction peaks.


## 3.3. SEM Analysis and DC Conductivity Measurements

Scanning electron microscopy (SEM) technique revealed that the ceramic material has particles with a range of micrometric sizes with plates-like morphology. For PANI-ES nanosized particles with morphologies similar to interconnected nanospheres were observed, which form the polymer nanofibers. Figures4, 5(a), and 5(b) show, respectively, the morphologies of alumina and PANI-ES. In the nanocomposite it was observed that polymerization of PANI-ES occurred on the α-Al2O3 plates by physical deposition (as suggested by FTIR analysis), being possible to observe in Figures 6(a)–6(c) the morphology of both materials combined in nanocomposite form.Figure 4
SEM image ofα-Al2O3.SEM image of PANI-ES with increase of (a) 31,000 and (b) 100,000 times.
(a)
(b)SEM images of PANI-ES/α-Al2O3 nanocomposite.
(a)
(b)
(c)An increasing about 1,300 times in nanocomposite DC electrical conductivity (0.24 S/cm) was verified when compared to the pure sample of PANI-ES [25]. This is surprising since alumina is an electrical insulator with DC electrical conductivity about 10−14 S/cm. The pure PANI-ES conductivity was found around 1.84
×
10
-
4 S/cm for Sanches et al. [25], as expected.We suggest that the most compact PANI-ES interface between theα-Al2O3 plates contributed significantly to increasing the nanocomposite DC electrical conductivity. The conductive polymer over the α-Al2O3 plates surface (percolation threshold) might promoted easier paths for the charge carriers. Zhang [8] obtained a conductive value of 0.17 S/cm for core-shell structured alumina-polyaniline particles. Michálek et al. [49] studied the electrical conductivity in alumina/multiwall carbon nanotubes (MWCNT) that obtained an increase from 10−14 S/cm (pure alumina) to 2.7
·
10
-
3 S/cm for composites. However, the DC electrical conductivity can decrease in the case of a better interaction between the composite components: Teoh et al. [50] synthesized nanofibers composite by oxidative polymerization of aniline with alumina nanofibers and the DC electrical conductivity decreased with increasing alumina nanofibers from 0.18 S/cm to 10−3 S/cm for alumina loading from 0% to 20%.


## 3.4. Le Bail Method Analysis

A process using iteratively the Rietveld decomposition formula for whole powder pattern decomposition (WPPD) purposes was first applied in 1988 [37] and called much later the “Le Bail method” or “Le Bail fit,” or “pattern matching” as well as “profile matching” in the FullProf Rietveld program [40]. In the original computer program first applying that method, arbitrarily all equal S
k
(
calc
)
2 values are first used, instead of using structure factors calculated from the atomic coordinates, resulting in “I
k
(
obs
)” which are then reinjected as new S
k
(
calc
)
2 values at the next iteration, while the usual profile and cell parameters (but not the scale) are refined by least squares. Equipartition of exactly overlapping reflections comes from the strictly equal result for Bragg peaks at the same angles which would have starting equal calculated intensities. Not starting from a set of all equal S
k
(
calc
)
2 values would produce I
k
(
obs
) values keeping the same original ratio for the exactly overlapping reflections. It is understandable that such an iterative process requires as good starting cell and profile parameters as the Rietveld method itself [51].To perform Le Bail method the crystal symmetry and unit cell for PANI and aluminum oxide obtained, respectively, by Evain et al. [43] and Lutterotti and Scardi [44] were used as input data. The refinement steps were followed by refining the peak width, refinement of a
,
b
,and  c and a
,
b
,
c
,
α
,
β, and γ. This sequence was addressed for both phases. Figure 7 shows the final refinement, with the observed (I
obs, black) and the calculated (I
calc, red) diffractograms, as well as the residual line (I
obs
-
I
calc, blue). Table 1 shows the refined parameters.Table 1
Comparison between the values found by Evain et al. (2002) [43] and Lutterotti and Scardi (1990) [44] with those found by PANI-ES and α-Al2O3, respectively, through Le Bail method.
Refined parameters
Evain et al., (2002) [43]
PANI-ES
Lutterotti and Scardi (1990) [44]
α-Al2O3
a (Å)
5.7328(1)
5.754363
4.7540(5)
4.756846
b (Å)
8.8866(2)
8.855334
4.7540(5)
4.756846
c (Å)
22.6889(6)
22.961094
12.9820(6)
12.966290
α (°)
82.7481(8)
84.222496
90
90
β (°)
84.5281(8)
84.180656
90
90
γ (°)
88.4739(11)
88.148727
120
120
V (Å3)
1141.3(4)
1160
254.1
254.0
Global average size (anisotr.) (Å)
—
41(10)
—
250(40)
Crystallite apparent size100 (Å)
—
46
—
140
Crystallite apparent  size010 (Å)
—
30
—
140
Crystallite apparent  size001 (Å)
—
35
—
90
R
wp (%)
9.3
R
p (%)
5.1
χ
2
6.6Figure 7
Le Bail method applied to nanocomposite.The refined parameters values ​​were compared with those obtained in literature [43, 44]. It is important to stress that the standard deviation appearing in the global average apparent size is calculated using the reciprocal lattice directions so it is a measure of the degree of anisotropy, not of the estimated error. The crystallite size projections for ES-PANI are showed in Figure 8(a). The crystallite shape can be described as a prolate ellipsoidal shape with its longer axis roughly parallel to [
110
] [25]. There was an average crystallite size around 41 Å with standard deviation (anisotropy) of 10 Å. There are a smaller apparent size of 30 and 35 Å in the [
010
] and [
001
] directions, respectively, and others almost equivalent (46 Å) along [
100
]. The crystallite size projections for α-Al2O3 are showed in Figure 8(b). There was an average crystallite size around 250 Å with standard deviation (anisotropy) of 40 Å. There is a largest apparent size of 140 Å in the [
100
] and [
010
] directions, and other smaller (90 Å) along [
001
]. Through Le Bail method it was verified that nanocomposite phases have kept its lattice parameters and provide structural information about crystallite size and shape.Crystallite shapes for (a) PANI-ES and (b)α-Al2O3.
(a)
(b)


## 4. Conclusions

We successfully obtained polyaniline emeraldine-salt form/α-aluminum oxide (PANI-ES/α-Al2O3) nanocomposite byin situ polymerization. XRD analysis showed that nanocomposite presents a semicrystalline pattern (with estimated crystallinity around 70%) with peaks related to both materials. SEM analysis showed that PANI-ES was polymerized over the α-Al2O3 plates.FTIR technique revealed that nanocomposite has characteristic absorption bands related to both materials, suggesting that nanocomposite has preserved the original structural characteristics of its constituents. Conducting polymer/inorganic nanocomposite can be classified into two types: physical deposition, in which the polymer is absorbed on the surface of inorganic particles, and chemical deposition, in which there is a covalent bond between them [11]. So, FTIR analysis showed that there was no chemical interaction between PANI-ES and α-Al2O3.The great contribution of this work is to obtain structural information using the Le Bail whole powder pattern decomposition method applied to a semicrystalline system consisting of semicrystalline polymeric/highly crystalline ceramic materials. The purpose of this work is also to promote this important structural characterization tool, which can be properly applied for semicrystalline materials. This method allowed the determination of cell parameters and crystallite size/shape for all phases. The refined cell parameters, so closed to the original values, showed that all phases have kept its structural characteristics after synthesis. For PANI-ES andα-Al2O3 there were, respectively, average crystallite sizes around 41 and 250 Å.With respect to conductivity measurements, this work showed that it is possible to increase the conductivity of polyaniline by synthesizing a nanocomposite using an insulating matrix. It was observed that the polymerization of PANI-ES overα-Al2O3 particles promoted an increasing of conductivity around 1,300 times when compared to pure sample of PANI-ES. To explain this increasing in conductivity, we suggested that the interface between PANI-ES/α-Al2O3 probably created easier paths for charge carriers in nanocomposite. We hope that the structural information provided in this study may be useful in the area of materials science and, more specifically, in several technological applications that require conducting nanocomposites with electrical conductivity in the obtained range.



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*Source: 375312-2015-02-09.xml*